CN102629283A - Simulation analysis method for effects of rotating part on flexible dynamics - Google Patents

Simulation analysis method for effects of rotating part on flexible dynamics Download PDF

Info

Publication number
CN102629283A
CN102629283A CN2011104256174A CN201110425617A CN102629283A CN 102629283 A CN102629283 A CN 102629283A CN 2011104256174 A CN2011104256174 A CN 2011104256174A CN 201110425617 A CN201110425617 A CN 201110425617A CN 102629283 A CN102629283 A CN 102629283A
Authority
CN
China
Prior art keywords
flexible
model
rotatable parts
beta
dynamics
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Granted
Application number
CN2011104256174A
Other languages
Chinese (zh)
Other versions
CN102629283B (en
Inventor
吕旺
薛孝补
杨立峰
朱海江
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Shanghai Institute of Satellite Engineering
Original Assignee
Shanghai Institute of Satellite Engineering
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Shanghai Institute of Satellite Engineering filed Critical Shanghai Institute of Satellite Engineering
Priority to CN2011104256174A priority Critical patent/CN102629283B/en
Publication of CN102629283A publication Critical patent/CN102629283A/en
Application granted granted Critical
Publication of CN102629283B publication Critical patent/CN102629283B/en
Active legal-status Critical Current
Anticipated expiration legal-status Critical

Links

Images

Landscapes

  • Management, Administration, Business Operations System, And Electronic Commerce (AREA)

Abstract

The invention discloses a simulation analysis method for effects of a rotating part on flexible dynamics. The simulation analysis method includes analyzing features of a large rotating part, and building a dynamic model of the large rotating part; performing structural dynamic analysis to flexible accessories of the large rotating part, generating a linearized vibration model described by a modal coordinate after modal truncation, building a multibody dynamic model with the flexible accessories according to a rigid body dynamic model; building a flexible satellite attitude dynamic and control system model based on the built models, and performing simulation by using the flexible satellite attitude dynamic and control system model; and performing time domain and frequency domain analysis to simulation data to obtain perturbation features. The simulation analysis method can be used not only for conformation of design results in attitude and obit control and dynamic design processes, but also for failure determination and inversion during obit operation. The simulation analysis method for the effects of the rotating part on flexible dynamics solves the practical engineering problem of the effects of the rotating part on flexible dynamics, and has the advantage that stability and reliability of platforms are improved.

Description

A kind of rotatable parts are to the simulating analysis of flexible kinetic effect
Technical field
The present invention relates to Structural Dynamics and dynamics, more particularly, relate to the simulating analysis of a kind of rotatable parts flexible kinetic effect.
Background technology
Development along with modern technologies; Pointing accuracy and degree of stability to satellite; And long-life and high reliability etc. require day by day to improve; Rotatable parts in the satellite and structure flexible appendage coupled vibrations more and more cause people's attention to effect of kinetics, and flexible Dynamic Modeling becomes the important topic that space industry is studied with analysis.
In flight and control procedure; Disturbing force (moment) and control (moment) not only can cause the change of position and attitude; And can evoke the elastic vibration of the flexible appendage in the rotatable parts, the elastic vibration of flexible appendage and then have influence on control accuracy and the load imaging stability of satellite again.The cyclic torque that particularly produces when rotatable parts causes flexible appendage easily and resonates during with the coupling of flexible appendage vibration frequency, has a strong impact on the operate as normal of satellite, can cause the flexible appendage fatigue damage when coupled vibrations is serious even also.Therefore, in dynamic analysis and controlling Design, must analyze and can emulation rotatable parts motion artifacts be coupled with accessory structure is flexible, and to the effect of kinetics degree.But also there is not such method in the prior art.
Summary of the invention
Lack the defective of analyzing when the objective of the invention is to overcome prior art, thereby a kind of simulating analysis accurately and rapidly is provided rotatable parts and flexible appendage generation coupling thereof.
For solving the problems of the technologies described above, the invention provides the simulating analysis of a kind of rotatable parts to flexible kinetic effect, comprising:
Step 1), the characteristic of large-scale rotatable parts is analyzed, set up the kinetic model of said large-scale rotatable parts;
Step 2), to rotatable parts with flexible appendage carry out the Structural Dynamics analysis, through generating the model of vibration that linearizing modal coordinate is described down after the mode truncation, have the many-body dynamics model of flexible appendage in conjunction with the rigid dynamics modelling;
Step 3), in step 1) and step 2) set up Flexible Satellite Attitude dynamics and control system model on the model based set up, utilize this model to carry out emulation;
Step 4), the emulated data that step 3) is obtained are carried out the time-domain and frequency-domain analysis, obtain perturbation features.
In the technique scheme, in described step 1), the kinetic model of said large-scale rotatable parts is the unbalancing value, static-unbalance of said rotatable parts perturbed force F and the moment T to whole star barycenter;
F = ω r 2 B j cos β j B j sin β j 0 , T = ω r 2 B d sin β d - z a B j cos β j B d cos β d + z a B j sin β j x a B j cos β j - y a B j sin β j
Wherein, B jBe static-unbalance size, B jBe static-unbalance phase place, B dBe unbalancing value size, β dBe unbalancing value phase place, [x a, y a, z a] be that RP is at body series coordinate, ω rBe the rotatable parts rotating speed.
In the technique scheme, described many-body dynamics model comprises:
Figure BSA00000638607500023
Wherein, ω is an angular velocity, v cBe mass center line speed; η is the mode variable, and Ω is the flexible appendage fundamental vibration frequency, and ξ is a flexible appendage vibration damping coefficient; BR, BT are respectively rotation, the translation coupling coefficient of the relative barycenter of flexible appendage, and F, T are respectively the dynamic and static imbalance of rotatable parts and cause perturbed force and moment.
The invention has the advantages that:
Can reflect real dynamic conditions accurately, the dynamics labile factor of rail control Subsystem Design scheme can be in time found and diagnosed out in the analysis of design time; Analysis in orbit can reappear in rail vibration situation fast and accurately, accurately locatees vibration cause, guarantees normal flight and service operation.
Description of drawings
Accompanying drawing 1 is the process flow diagram of method of the present invention in one embodiment;
Accompanying drawing 2 is a Coupled Dynamics realistic model framework related in the embodiments of the invention.
Embodiment
Below in conjunction with accompanying drawing and embodiment the present invention is further specified.
With reference to figure 1, method of the present invention may further comprise the steps:
Step 1), the characteristic of large-scale rotatable parts is analyzed, set up the kinetic model of said large-scale rotatable parts.
Rotatable parts have generally all carried out balancing when appearing on the scene, but still have remaining static-unbalance and remaining unbalancing value, and described remaining static-unbalance and remaining unbalancing value are the important indicators of examination rotatable parts dynamic performance.The disturbance torque of rotatable parts can be caused by remaining static-unbalance and remaining unbalancing value, therefore, the rotatable parts kinetic model that is used to export disturbance torque can be created by remaining static-unbalance and remaining unbalancing value.Said remaining static-unbalance and unbalancing value generally provide with the form of mould and phase place, in addition, when providing remaining static-unbalance with amount, must confirm reference point locations, generally it are selected in the nominal barycenter place of rotatable parts.The input quantity of the kinetic model that will create as shown in the table:
Figure BSA00000638607500031
Table 1
Unbalancing value, static-unbalance can be expressed as respectively the perturbed force F and the moment T of whole star barycenter:
F = ω r 2 B j cos β j B j sin β j 0 , T = ω r 2 B d sin β d - z a B j cos β j B d cos β d + z a B j sin β j x a B j cos β j - y a B j sin β j - - - ( 1 )
The kinetic model that the expression formula of above-mentioned perturbed force F and moment T is just set up for said large-scale rotatable parts.
Step 2), to rotatable parts with flexible appendage carry out the Structural Dynamics analysis, through generating the model of vibration that linearizing modal coordinate is described down after the mode truncation, have the many-body dynamics model of flexible appendage in conjunction with the rigid dynamics modelling.
In this step, on classical mechanics theoretical foundation, use D'Alembert's principle and principle of conservation of momentum and derive flexible kinetics equation, be i.e. rigid dynamics model (like first, second equation in the hereinafter formula (2)); The Application of Lagrange's Equations and the principle of virtual work are set up the mathematical model of flexible appendage elastic vibration, i.e. flexible appendage elastic vibration equation (like the 3rd equation in the hereinafter formula (2)).Flexible appendage elastic vibration equation and flexible translation, rotational power equations simultaneousness are obtained flexible dynamics fundamental equation, i.e. many-body dynamics equation.The application constraint modal method is done mode truncation to fundamental equation, asks for approximate solution, and the fundamental equation that obtains under the hybrid coordinate is following:
Figure BSA00000638607500043
Wherein, ω is an angular velocity, v cBe mass center line speed; η is the mode variable, and Ω is the flexible appendage fundamental vibration frequency, and ξ is a flexible appendage vibration damping coefficient; BR, BT are respectively rotation, the translation coupling coefficient of the relative barycenter of flexible appendage, and F, T are respectively the dynamic and static imbalance of rotatable parts and cause perturbed force and moment.
Step 3), in step 1) and step 2) set up Flexible Satellite Attitude dynamics and control system model on the model based set up, utilize this model to carry out emulation.
As shown in Figure 2, described Flexible Satellite Attitude dynamics and control system model comprise rigid dynamics model, flexible appendage model of vibration, rotatable parts moment model and control system model.Wherein, described control system model is used for other models are done FEEDBACK CONTROL, and this model can pass through existing techniques in realizing.
In the simulation process, the rotatable parts moment model generates time dependent perturbed force F and moment T, sends to the rigid dynamics model; The rigid dynamics model comprises translation and rotational power is learned model, and input quantity is the mode variable n of rotatable parts perturbed force F, disturbance torque T and flexible appendage vibration, and output quantity is Eulerian angle Euler, angular velocity omega and mass center line speed v cThe flexible appendage model of vibration receives angular velocity omega and the mass center line speed v from the rigid dynamics model c, output modalities coordinate n returns to the rigid dynamics model; That the control system model comprises is definite, control and topworks's model, gathers Eulerian angle Euler and angular velocity omega, with the angular momentum exchanged form to carrying out FEEDBACK CONTROL.
Step 4), the emulated data of said Flexible Satellite Attitude dynamics and control system model is analyzed and assessed.
The resulting emulated data of step 3) (in the rail data) is carried out time and frequency domain analysis, obtain perturbation features.The time-domain analysis fundamental purpose be investigate receive the rotatable parts disturbance after, whether still satisfy index request, draw the rotatable parts disturbance to flexible effect of kinetics degree.Function is analyzed in the fast Fourier transform (FFT) of the main Origin Pro software capable of using of frequency-domain analysis, high pass (High Pass), low pass (Low Pass), band logical (Band Pass), band resistance (Band Block) etc.; Obtain the spectral characteristic of data, be used for the anti-characteristic that pushes away disturbing source and bang path.
Obtain rotatable parts to flexible kinetic effect degree after, those skilled in the art combine existing knowledge, can be according to the design of these information guidings or in the rail fault analysis.
Method of the present invention can be used in rail control and the dynamics Design process design result being verified, also is used in the fault verification and the inverting of rail run duration.
Obviously, those skilled in the art can carry out various changes and distortion to the present invention and not break away from the spirit and scope of the present invention.Like this, if these modifications and distortion belong within the scope of claim of the present invention and equivalent technologies thereof, then the present invention also is intended to comprise these changes and is out of shape interior.

Claims (3)

1. rotatable parts comprise the simulating analysis of flexible kinetic effect:
Step 1), the characteristic of large-scale rotatable parts is analyzed, set up the kinetic model of said large-scale rotatable parts;
Step 2), to rotatable parts with flexible appendage carry out the Structural Dynamics analysis, through generating the model of vibration that linearizing modal coordinate is described down after the mode truncation, have the many-body dynamics model of flexible appendage in conjunction with the rigid dynamics modelling;
Step 3), in step 1) and step 2) set up Flexible Satellite Attitude dynamics and control system model on the model based set up, utilize this model to carry out emulation;
Step 4), the emulated data that step 3) is obtained are carried out the time-domain and frequency-domain analysis, obtain perturbation features.
2. rotatable parts according to claim 1 are to the simulating analysis of flexible kinetic effect; It is characterized in that; In described step 1), the kinetic model of said large-scale rotatable parts is the unbalancing value, static-unbalance of said rotatable parts perturbed force F and the moment T to whole star barycenter;
F = ω r 2 B j cos β j B j sin β j 0 , T = ω r 2 B d sin β d - z a B j cos β j B d cos β d + z a B j sin β j x a B j cos β j - y a B j sin β j
Wherein, B jBe static-unbalance size, β jBe static-unbalance phase place, B dBe unbalancing value size, β dBe unbalancing value phase place, [x a, y a, z a] be that RP is at body series coordinate, ω rBe the rotatable parts rotating speed.
3. rotatable parts according to claim 2 is characterized in that to the simulating analysis of flexible kinetic effect described many-body dynamics model comprises:
Figure FSA00000638607400013
Wherein, ω is an angular velocity, v cBe mass center line speed; η is the mode variable, and Ω is the flexible appendage fundamental vibration frequency, and ξ is a flexible appendage vibration damping coefficient; BR, BT are respectively rotation, the translation coupling coefficient of the relative barycenter of flexible appendage, and F, T are respectively the dynamic and static imbalance of rotatable parts and cause perturbed force and moment.
CN2011104256174A 2011-12-15 2011-12-15 Simulation analysis method for effects of rotating part on flexible dynamics Active CN102629283B (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
CN2011104256174A CN102629283B (en) 2011-12-15 2011-12-15 Simulation analysis method for effects of rotating part on flexible dynamics

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
CN2011104256174A CN102629283B (en) 2011-12-15 2011-12-15 Simulation analysis method for effects of rotating part on flexible dynamics

Publications (2)

Publication Number Publication Date
CN102629283A true CN102629283A (en) 2012-08-08
CN102629283B CN102629283B (en) 2013-11-27

Family

ID=46587543

Family Applications (1)

Application Number Title Priority Date Filing Date
CN2011104256174A Active CN102629283B (en) 2011-12-15 2011-12-15 Simulation analysis method for effects of rotating part on flexible dynamics

Country Status (1)

Country Link
CN (1) CN102629283B (en)

Cited By (6)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN106483872A (en) * 2015-08-26 2017-03-08 上海宇航系统工程研究所 The flexible solar wing of simulation drives the precision judge method of dynamics simulation testing stand
CN103970964B (en) * 2014-05-23 2017-05-24 哈尔滨工业大学 Flexible satellite modal parameter in-orbit identification method
CN107992660A (en) * 2017-11-24 2018-05-04 上海航天控制技术研究所 A kind of Spacecraft method of integrated modeling
CN108133096A (en) * 2017-12-20 2018-06-08 大连交通大学 Hitch dynamic reliability Forecasting Methodology based on MBD and SVM
CN109471424A (en) * 2018-12-04 2019-03-15 上海航天控制技术研究所 A kind of big angular momentum rotatable parts ground simulation test macro and method
CN109507875A (en) * 2019-01-08 2019-03-22 哈尔滨工业大学 A kind of Euler's spinning satellite attitude maneuver passs rank saturation PID control method

Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US6024327A (en) * 1997-05-15 2000-02-15 Electronics And Telecommunications Research Institute Method and apparatus for intelligent attitude and orbit control onboard a satellite
CN101814107A (en) * 2010-05-06 2010-08-25 哈尔滨工业大学 Satellite dynamics simulation system and method based on satellite dynamics model library

Patent Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US6024327A (en) * 1997-05-15 2000-02-15 Electronics And Telecommunications Research Institute Method and apparatus for intelligent attitude and orbit control onboard a satellite
CN101814107A (en) * 2010-05-06 2010-08-25 哈尔滨工业大学 Satellite dynamics simulation system and method based on satellite dynamics model library

Non-Patent Citations (2)

* Cited by examiner, † Cited by third party
Title
刘莹莹等: "《挠性多体航天器姿态动力学建模与分析》", 《飞行力学》 *
王钦等: "《带挠性附件的航天器结构-姿态耦合动力学》", 《上海航天》 *

Cited By (9)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN103970964B (en) * 2014-05-23 2017-05-24 哈尔滨工业大学 Flexible satellite modal parameter in-orbit identification method
CN106483872A (en) * 2015-08-26 2017-03-08 上海宇航系统工程研究所 The flexible solar wing of simulation drives the precision judge method of dynamics simulation testing stand
CN106483872B (en) * 2015-08-26 2018-12-28 上海宇航系统工程研究所 Simulate the precision judge method of flexible solar wing driving dynamics simulation testing stand
CN107992660A (en) * 2017-11-24 2018-05-04 上海航天控制技术研究所 A kind of Spacecraft method of integrated modeling
CN107992660B (en) * 2017-11-24 2021-02-05 上海航天控制技术研究所 Flexible spacecraft integrated modeling method
CN108133096A (en) * 2017-12-20 2018-06-08 大连交通大学 Hitch dynamic reliability Forecasting Methodology based on MBD and SVM
CN108133096B (en) * 2017-12-20 2021-04-09 大连交通大学 Coupler dynamic reliability prediction method based on MBD and SVM
CN109471424A (en) * 2018-12-04 2019-03-15 上海航天控制技术研究所 A kind of big angular momentum rotatable parts ground simulation test macro and method
CN109507875A (en) * 2019-01-08 2019-03-22 哈尔滨工业大学 A kind of Euler's spinning satellite attitude maneuver passs rank saturation PID control method

Also Published As

Publication number Publication date
CN102629283B (en) 2013-11-27

Similar Documents

Publication Publication Date Title
CN102629283B (en) Simulation analysis method for effects of rotating part on flexible dynamics
Cavagna et al. Application of Navier–Stokes simulations for aeroelastic stability assessment in transonic regime
Chakraborty et al. Nonlinear region of attraction analysis for flight control verification and validation
Wu et al. Linear and nonlinear aeroelastic analysis frameworks for cable-supported bridges
CN101497374B (en) Method for producing disturbing torque to satellite using equivalent simulation of flexible accessory vibration by flywheel
Howison et al. Aeroelastic analysis of a wind turbine blade using the harmonic balance method
Kersken et al. Nonreflecting boundary conditions for aeroelastic analysis in time and frequency domain 3D RANS solvers
Zhao et al. Prediction of transient responses of a folding wing during the morphing process
CN102609561B (en) Simulation method for influence of rotation part on flexible dynamics
Raveh et al. Analyses for the second aeroelastic prediction workshop using the EZNSS code
Fischer et al. Control design for mechanical hardware‐in‐the‐loop operation of dynamometers for testing full‐scale drive trains
Sun et al. Review on the theories and applications of dynamic condensation and component mode synthesis methods in solving FEM-based structural dynamics
Mavriplis et al. Extensions of time spectral methods for practical rotorcraft problems
Bartels Development, verification and use of gust modeling in the nasa computational fluid dynamics code fun3d
Zhou et al. Efficient nonlinear aeroelastic analysis of a morphing wing via parameterized fictitious mode method
CN104361145B (en) Rotor dynamics modeling method based on axle closely attached coordinate system
Liu et al. An efficient numerical method for dynamic analysis of polygonal plate under moving loads
Kassem et al. Transonic flutter analysis using a fully coupled density based solver for inviscid flow
CN103473401B (en) Wind turbine model based on PSASP and power disturbance realistically displayed method thereof
Sheng et al. CFD/CSD Coupled Simulations for a Helicopter Rotor in Forward and Maneuvering Flight
Marsden et al. Transient and limit cycle simulation of a nonlinear aeroelastic system
Yun et al. Application of ground flutter emulation test technique for the passive flutter suppression effect validation
Fancello et al. Helicopter rotor sailing by non-smooth dynamics co-simulation
Shuaishuai et al. Nonlinear system identification framework of folding fins with freeplay using backbone curves
KR20140084645A (en) Computer readable recording medium for recording flight dynamic analysis/simulation program for helicopter fbw system development

Legal Events

Date Code Title Description
C06 Publication
PB01 Publication
C10 Entry into substantive examination
SE01 Entry into force of request for substantive examination
C53 Correction of patent of invention or patent application
CB03 Change of inventor or designer information

Inventor after: Lv Wang

Inventor after: Xue Xiaobu

Inventor after: Chen Jing

Inventor after: Yang Lifeng

Inventor after: Zhu Haijiang

Inventor before: Lv Wang

Inventor before: Xue Xiaobu

Inventor before: Yang Lifeng

Inventor before: Zhu Haijiang

COR Change of bibliographic data

Free format text: CORRECT: INVENTOR; FROM: LV WANG XUE XIAOBU YANG LIFENG ZHU HAIJIANG TO: LV WANG XUE XIAOBU CHEN JING YANG LIFENG ZHU HAIJIANG

C14 Grant of patent or utility model
GR01 Patent grant