CN114383874A - Large-scale structure modal testing method - Google Patents

Large-scale structure modal testing method Download PDF

Info

Publication number
CN114383874A
CN114383874A CN202111510347.7A CN202111510347A CN114383874A CN 114383874 A CN114383874 A CN 114383874A CN 202111510347 A CN202111510347 A CN 202111510347A CN 114383874 A CN114383874 A CN 114383874A
Authority
CN
China
Prior art keywords
sensor
modal
coordinate system
scale structure
excitation
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.)
Pending
Application number
CN202111510347.7A
Other languages
Chinese (zh)
Inventor
周昊天
张一凡
王大为
王京城
杨丰福
张亚林
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.)
CETC 54 Research Institute
Original Assignee
CETC 54 Research Institute
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 CETC 54 Research Institute filed Critical CETC 54 Research Institute
Priority to CN202111510347.7A priority Critical patent/CN114383874A/en
Publication of CN114383874A publication Critical patent/CN114383874A/en
Pending legal-status Critical Current

Links

Images

Classifications

    • GPHYSICS
    • G01MEASURING; TESTING
    • G01MTESTING STATIC OR DYNAMIC BALANCE OF MACHINES OR STRUCTURES; TESTING OF STRUCTURES OR APPARATUS, NOT OTHERWISE PROVIDED FOR
    • G01M99/00Subject matter not provided for in other groups of this subclass
    • G01M99/004Testing the effects of speed or acceleration
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01HMEASUREMENT OF MECHANICAL VIBRATIONS OR ULTRASONIC, SONIC OR INFRASONIC WAVES
    • G01H17/00Measuring mechanical vibrations or ultrasonic, sonic or infrasonic waves, not provided for in the preceding groups
    • GPHYSICS
    • G06COMPUTING; CALCULATING OR COUNTING
    • G06FELECTRIC DIGITAL DATA PROCESSING
    • G06F17/00Digital computing or data processing equipment or methods, specially adapted for specific functions
    • G06F17/10Complex mathematical operations
    • G06F17/16Matrix or vector computation, e.g. matrix-matrix or matrix-vector multiplication, matrix factorization
    • GPHYSICS
    • G06COMPUTING; CALCULATING OR COUNTING
    • G06FELECTRIC DIGITAL DATA PROCESSING
    • G06F30/00Computer-aided design [CAD]
    • G06F30/10Geometric CAD
    • GPHYSICS
    • G06COMPUTING; CALCULATING OR COUNTING
    • G06FELECTRIC DIGITAL DATA PROCESSING
    • G06F30/00Computer-aided design [CAD]
    • G06F30/20Design optimisation, verification or simulation
    • G06F30/23Design optimisation, verification or simulation using finite element methods [FEM] or finite difference methods [FDM]
    • GPHYSICS
    • G08SIGNALLING
    • G08CTRANSMISSION SYSTEMS FOR MEASURED VALUES, CONTROL OR SIMILAR SIGNALS
    • G08C17/00Arrangements for transmitting signals characterised by the use of a wireless electrical link
    • G08C17/02Arrangements for transmitting signals characterised by the use of a wireless electrical link using a radio link
    • GPHYSICS
    • G06COMPUTING; CALCULATING OR COUNTING
    • G06FELECTRIC DIGITAL DATA PROCESSING
    • G06F2119/00Details relating to the type or aim of the analysis or the optimisation
    • G06F2119/14Force analysis or force optimisation, e.g. static or dynamic forces

Landscapes

  • Engineering & Computer Science (AREA)
  • Physics & Mathematics (AREA)
  • General Physics & Mathematics (AREA)
  • Theoretical Computer Science (AREA)
  • Geometry (AREA)
  • Computational Mathematics (AREA)
  • Mathematical Optimization (AREA)
  • Mathematical Physics (AREA)
  • Pure & Applied Mathematics (AREA)
  • Mathematical Analysis (AREA)
  • General Engineering & Computer Science (AREA)
  • Evolutionary Computation (AREA)
  • Data Mining & Analysis (AREA)
  • Computer Hardware Design (AREA)
  • Databases & Information Systems (AREA)
  • Computing Systems (AREA)
  • Software Systems (AREA)
  • Algebra (AREA)
  • Computer Networks & Wireless Communication (AREA)
  • Testing Of Devices, Machine Parts, Or Other Structures Thereof (AREA)

Abstract

The invention provides a large-scale structure modal testing method, and belongs to the field of vibration testing. The method comprises the steps of optimizing and analyzing the position of the sensor, fixing sensor equipment, establishing the relation between the position direction of the sensor and a geometric model, acquiring and recording data, processing the data, identifying modal parameters and the like. The invention adopts the sensor with wireless transmission function to measure, thus reducing the experiment preparation time; the three-way micro-electromechanical acceleration sensor integrating the inclinometer and the positioning device is adopted, so that the cost is low, and the connection with a geometric model is conveniently established; and a step excitation method is adopted, so that the implementation difficulty is low.

Description

Large-scale structure modal testing method
Technical Field
The invention relates to a large-scale structure modal testing method, and belongs to the field of mechanical structure and vibration testing.
Background
The modality information includes three elements: natural frequency, modal damping ratio, and mode shape. The modal information reflects the inherent vibration characteristics of the structure itself, and is an important index that must be considered in the design, processing and manufacturing of large structures. In practical engineering, besides applying computer simulation technology, determining the mode of a large-scale structure by an experimentally measured method is also an essential important means.
Modal testing can be roughly divided into three forms according to the excitation form: sine sweep frequency, pulse excitation and step excitation. The sine sweep is a single frequency excitation of the structure by a vibration exciter or a vibration table, and the excitation is in a sine wave form, and the excitation frequency changes along with time. When the excitation frequency is close to the natural frequency of the structure, the structure resonates, the response amplitude is obviously increased, and the relevant modal parameters can be determined. Pulsed and stepped excitation is achieved by hammering or displacing a boundary change to elastically deform the structure and then releasing abruptly to obtain a free response of the structure. The structural modal parameters are obtained by the free response of the structure. In modal testing, the structural response may be displacement, velocity, acceleration, strain, and the like. Acceleration response is often used in practical engineering applications.
For a large structure, large excitation equipment is needed by adopting sweep frequency excitation, and displacement boundary conditions of the structure need to be properly constrained, so that the implementation difficulty is high, the cost is high, and the experimental period is long. The structure can be effectively excited by adopting a pulse or step excitation mode, but a large-scale space structure usually pays attention to vibration characteristics in all directions, so that a three-way sensor is needed. The traditional test method needs acquisition equipment with a large number of channels, so that the cost is high; the three-way sensor has more wire harnesses, is easy to be interfered, and has longer experiment preparation period.
Disclosure of Invention
Aiming at the defects of the prior art, the invention provides the large structure modal testing method, which can test the natural frequency of large structures in various forms, and has the advantages of low cost and easy implementation.
In order to achieve the purpose, the invention adopts the technical scheme that:
a large-scale structure modal test method comprises the following steps:
(1) carrying out modal analysis on a large-scale structure to be tested to obtain initial natural frequency and vibration mode;
(2) according to the preliminary vibration mode obtained in the step (1), determining the installation position of the sensor by comparing vibration mode results in the concerned frequency, and installing the sensor at a position with a large amplitude in the vibration mode; a three-axis acceleration sensor, an inclinometer, a positioning device and a wireless connecting device are arranged in the sensor;
(3) establishing a relation between the sensor position direction and the geometric model;
(4) step excitation is applied to the large-scale structure, the amplitude of acceleration response is monitored through the information processing computer, excitation is performed again when the acceleration response is attenuated, the excitation is repeated for multiple times, and response data of each sensor is recorded through the information processing computer;
(5) and processing the data according to the response data of the sensor and the relation between the sensor position direction and the geometric model to obtain the modal parameters of the large-scale structure.
Further, the specific mode of the step (3) is as follows:
(301) establishing a global coordinate system in an information processing computer, and importing a geometric model of a large-scale structure;
(302) determining the position coordinate and the attitude direction of the sensor by utilizing a positioning device and an inclinometer which are arranged in the sensor;
(303) and establishing a relation between the sensor position direction and the large-scale structure geometric model, wherein the relation comprises the specific position of the sensor measuring point in the large-scale structure geometric model and a rotation matrix from a sensor coordinate system to a whole coordinate system.
Further, in the step (4), firstly, time synchronization is carried out on each sensor by utilizing the time service function of the positioning device; the specific way of applying the step excitation is to excite the large-scale structure in three directions respectively, and at least 10 times of effective free attenuation is recorded in each excitation direction; and after the data recording of each direction is completed, the excitation of the next direction is carried out.
Further, the specific mode of the step (5) is as follows:
(501) obtaining the acceleration response of the sensor under the global coordinate system according to the rotation matrix from the sensor coordinate system to the global coordinate system:
Figure BDA0003405031190000021
in the formula, RnGIs a rotation matrix, vector, from the sensor coordinate system to the global coordinate system
Figure BDA0003405031190000022
For the acceleration response of the sensor in the global coordinate system,
Figure BDA0003405031190000023
the acceleration response of the sensor under the coordinate system of the sensor is obtained;
(502) selecting a sensor as a reference sensor according to the initial natural frequency obtained in the step (1), so that a power spectrogram of the response data of the reference sensor comprises natural frequency components of each order; carrying out Fourier transform on the response data of the reference sensor, wherein each extreme point corresponds to the inherent frequency of different orders;
(503) decomposing response data of the reference sensor to obtain modal responses of all orders, enveloping the modal responses of all orders and carrying out exponential curve fitting to obtain modal damping ratios of different orders; wherein the form of the exponential curve is as follows:
x=Ae-σt=Ae-2πfξt
xe=Ae-σt=Ae-2πfξte=Ae-σt=Ae-2πfξt
in the formula, xeExtracting envelope data on acceleration response, wherein A is a signal amplitude, f is the natural frequency of the order, and xi is a modal damping ratio to be solved;
(504) decomposing the response data of each sensor to obtain concerned modal responses of each order; averaging root mean square values obtained by the same sensors, the same direction, the same order and different excitation orders according to the excitation orders to obtain vibration mode components of the corresponding sensors, the corresponding directions and the corresponding orders; and carrying out maximum value normalization on the vibration mode components of different sensors and the same order to obtain the vibration modes of different orders of the large-scale structure.
Compared with the prior art, the invention has the beneficial effects that:
1. the invention aims at the characteristic of large scale of a large structure, adopts the sensor with the wireless transmission function to carry out measurement, can realize wireless measurement and automatically acquire the position and the direction of the sensor, is easy to implement in the test process, does not need wiring and wire arrangement, and can obviously reduce the test time.
2. Aiming at the problem that a large structure requires attention to vibration modes in three directions, the three-direction micro-electromechanical acceleration sensor integrating the inclinometer and the positioning device is adopted, so that the cost is low, and the connection with a geometric model is conveniently established.
3. Aiming at the problem that a large-scale structure is difficult to excite by a vibration exciter, the invention adopts displacement step to excite, and the excitation form is simple and easy to realize.
Drawings
Fig. 1 is a schematic structural diagram of a large-scale structural modal testing system according to an embodiment of the present invention.
Fig. 2 is a schematic view of the installation position of the sensor in the embodiment of the present invention.
Fig. 3 is a graph of the acceleration response spectrum of the sensor at the ball node 4 in the X direction according to the embodiment of the present invention.
Fig. 4 is a graph of the X-direction acceleration response envelope of the sensor at the ball node 4 in an embodiment of the present invention.
Detailed Description
In order to make the objects, technical solutions and advantages of the present invention more apparent, the present invention will be described in further detail with reference to the accompanying drawings and specific embodiments, wherein the exemplary embodiments and descriptions thereof are only used for explaining the present invention and are not meant to limit the present invention.
A large-scale structural mode testing method, a testing system thereof is shown in fig. 1, the testing system comprises:
the smart sensor device 1. The sensor equipment is internally provided with a three-axis acceleration sensor, an inclinometer, a GPS or Beidou positioning device, a WiFi or Bluetooth or other wireless connection devices. The intelligent sensor equipment is internally provided with related software which can carry out data acquisition and data preprocessing on the sensor and send the sensor data to the wireless connection switch through a built-in wireless device according to a wireless protocol.
A wireless connection switch 2. The device provides a wireless connection convergence function, and converges the structural response information acquired by the sensor to the information processing computer through the network. The wireless network switch wireless connection protocol needs to be compatible with the sensor wireless connection protocol.
An information processing computer 3. The computer is connected with the wireless network switch and can receive the data of each sensor gathered by the switch. And the information processing computer is provided with special software for processing the sensor data and identifying the large-scale structure modal parameters.
The method mainly comprises the following steps:
(1) and (5) optimizing and analyzing the position of the sensor. And carrying out modal analysis on the structure to be tested by finite element mechanical analysis software or a theoretical method to obtain initial natural frequency and vibration mode.
(2) The sensor device is fixed. And determining the installation position of the sensor by comparing the vibration mode results in the concerned frequency, and fixing the sensor equipment to the corresponding position of the structure. The sensor mounting position should be avoided from being mounted at a vibration mode node position, a vibration mode amplitude smaller position, and a position with larger structural rigidity is selected as far as possible. The fixing mode of the sensor is firm and reliable, the tool can be designed independently for clamping and fixing the sensor, and the tool can be mounted on the structure through bolts, hoops and the like.
The method adopts wireless sensor equipment, adopts a wireless transmission mode for data transmission, and can automatically report the posture and the position of the wireless sensor equipment by arranging an inclinometer and a positioning device in the wireless sensor equipment.
(3) And establishing the relation between the position direction of the sensor and the geometric model of the large-scale structure to be measured according to the attitude direction and the position information reported by the sensor. Firstly, an overall coordinate system is established in an information processing computer, a structural geometric model is imported, then the position coordinates and the attitude direction of a sensor are determined by utilizing special software preinstalled in the information processing computer and a positioning device and an inclinometer which are built in the sensor, and finally the relationship between the position direction of the sensor and the structural geometric model is established. The relationship includes the specific location of the sensor measurement points in the structural geometric model and the rotation matrix of the sensor coordinate system to the global coordinate system. Wherein, the rotation matrix from the sensor coordinate system to the global coordinate system can be a transformation matrix in Euler or Kaldo form.
(4) And (6) data acquisition and recording. The method comprises the steps of firstly synchronizing the time of sensors by using the time service function of a GPS or Beidou positioning device, then recording the acceleration data of each sensor by using special software preinstalled in an information processing computer, applying step excitation to a mechanism while recording the data and adding the amplitude of acceleration response in the software, exciting again when the acceleration response is attenuated, and repeating for many times.
Preferably, recording is stopped after more than 10 effective free decay responses have been recorded. The excitation direction was changed and the recording of the sensor acceleration response was resumed, stopping after 10 effective free decay responses were reached. The above steps are repeated until the structure has been excited in all three directions.
(5) Data processing and modal parameter identification. After obtaining the acceleration response of each sensor in three directions, obtaining the acceleration response of the sensor in the global coordinate system according to the rotation matrix between the coordinate system of each sensor and the global coordinate system obtained in the step (3), wherein a specific transformation formula is as follows:
Figure BDA0003405031190000051
in the formula, RnGIs a rotation matrix, vector, from the local coordinate system of the sensor to the global coordinate system
Figure BDA0003405031190000052
For the acceleration response of the acceleration sensor under the global coordinate system,
Figure BDA0003405031190000053
is the acceleration response of the sensor in its own coordinate system.
Selecting sensor data as reference data, wherein the power spectrogram of the sensor response data comprises natural frequency components of each order, and the reference value of the modal frequency can refer to the natural frequency obtained by the modal analysis in the step (1). And carrying out Fourier transform on the reference sensor data, wherein each extreme point corresponds to the natural frequency of different orders of the structure.
And decomposing the response data of the reference sensor to obtain modal responses of all orders, and enveloping and carrying out exponential curve fitting on the modal responses of all orders to obtain modal damping ratios of different orders of the structure. The exponential curve is of the form:
x=Ae-σt=Ae-2πfξt
xe=Ae-σt=Ae-2πfξte=Ae-σt=Ae-2πfξt
wherein x iseAnd extracting envelope data on the acceleration response, wherein A is a signal amplitude, f is a natural frequency of the order, and xi is a modal damping ratio to be solved.
And decomposing the response data of each sensor to obtain concerned modal response of each order. According to the excitation sequence, averaging the root mean square values obtained by the same sensor, the same direction, the same order and different excitation sequences to obtain the vibration mode components of the sensor, the direction and the order. And performing the same processing on all sensor data to obtain vibration mode components of all sensors, all directions and the concerned order. And maximum value normalization is carried out on the vibration mode components of different sensors and the same order, so that the vibration modes of different structures and different orders can be obtained.
In the step (5), when the data of each sensor is decomposed, the calculation parameters are ensured to be consistent, and the modal responses of each order obtained by decomposition are equal in quantity; the algorithm used for the sensor data decomposition can be empirical mode decomposition, variational mode decomposition, wavelet decomposition and the like; when the root mean square value is solved for the modal responses of the same order of different sensors, the number of the selected data points is ensured to be the same.
Preferably, the sensor reference data amplitude in step (5) should not be too low.
In the following, a large structure is taken as an example, and the large structure is shown in fig. 2 and is a space truss structure. The modal testing method of the structure is as follows:
(1) modal analysis is carried out on the truss structure through finite element mechanical analysis software to obtain initial natural frequency and vibration mode, and installation positions of the sensors are determined to be positions of the ball nodes 4, 5 and 6 in the diagram 2 through the analysis.
(2) The sensor device is fixed. And (3) fixing the sensor equipment to the corresponding position of the structure according to the determined sensor installation position in the step (1).
(3) Sensor position coordinates are established. And importing a truss structure geometric model into computer special software, and establishing an overall coordinate system. The position coordinates and the orientation of the sensor are determined by using special software pre-installed in an information processing computer and a positioning device and an inclinometer built in the sensor, for example, the sensor at the ball node 4 has the coordinates of [ -3232,1179, -3232] in the space, and the coordinates are basically coincident with the ball node in the geometric model, so that the response of the sensor can be used for representing the response of the ball node in the geometric model. The included angle of the sensor and the Y-axis is 45 degrees.
(4) The acceleration data of each sensor is recorded by using special software pre-installed in an information processing computer, and step excitation is applied to the mechanism while the data is recorded, so that the effective excitation is carried out for 10 times in total.
(5) And (4) obtaining acceleration responses of the three sensors under the global coordinate system according to the transformation matrix between the coordinate system of each sensor and the global coordinate system obtained in the step (3) after obtaining the acceleration responses of the sensors. Taking the sensor at the ball node 4 as an example, the euler X-Y-Z coordinate rotation transformation matrix corresponding to the sensor is an expression, so that the sensor responds as follows under the overall coordinate system:
Figure BDA0003405031190000061
Figure BDA0003405031190000062
the sensor at the ball node 4 is selected as a reference, and the X-direction response Fourier transform spectrum of the sensor is shown in FIG. 3. As can be seen from the figure, the first three natural frequencies are 1.67 Hz, 3.18 Hz and 6.04Hz respectively. The X-direction data of the sensor is decomposed to obtain the first three-order modal responses, and the first order is taken as an example, and the single step response is shown in fig. 4. Obtaining an exponential envelope curve expression x according to response fitting in the graphe=Ae-σt=Ae-2πfξt=e-2π×1.67×0.0098×tTherefore, the first-order modal damping ratio is 0.98%.
And decomposing the response data of each sensor to obtain concerned modal response of each order. According to the excitation sequence, solving the root mean square value of the modal response of the same order of the three sensors, and averaging the root mean square values obtained by the same sensors, the same direction, the same order and different excitation sequences to obtain the vibration mode components of the sensor, the direction and the order. The same processing is carried out on all three sensor data, and vibration mode components of all sensors, all directions and the concerned orders are obtained. And maximum value normalization is carried out on the vibration mode components of the three sensors and the same order, so that the vibration modes with different orders of structures can be obtained.
In this example, the first order mode matrix is
Figure BDA0003405031190000071
The matrix has a first row of X-direction component, a second row of Y-direction component, and a third row of Z-direction component, wherein the first row is sensor mode component at ball node 4, the second row is sensor mode component at ball node 5, and the third row is sensor mode componentIs the sensor mode shape component at the ball node 6.
In a word, the invention adopts the sensor with the wireless transmission function to measure, thus reducing the experiment preparation time; the three-way micro-electromechanical acceleration sensor integrating the inclinometer and the positioning device is adopted, so that the cost is low, and the connection with a geometric model is conveniently established; and a step excitation method is adopted, so that the implementation difficulty is low.
The above-mentioned embodiments are intended to illustrate the objects, technical solutions and advantages of the present invention in further detail, and it should be understood that the above-mentioned embodiments are only illustrative of the present invention and are not intended to limit the scope of the present invention, and any modifications, equivalents, improvements and the like made within the spirit and principle of the present invention should be included in the scope of the present invention.

Claims (4)

1. A large-scale structure modal testing method is characterized by comprising the following steps:
(1) carrying out modal analysis on a large-scale structure to be tested to obtain a primary natural frequency and a primary vibration mode;
(2) according to the preliminary vibration mode obtained in the step (1), determining the installation position of the sensor by comparing vibration mode results in the concerned frequency, and installing the sensor at a position with a large amplitude in the vibration mode; a three-axis acceleration sensor, an inclinometer, a positioning device and a wireless connecting device are arranged in the sensor;
(3) establishing a relation between the sensor position direction and the geometric model;
(4) step excitation is applied to the large-scale structure, the amplitude of acceleration response is monitored through the information processing computer, excitation is performed again when the acceleration response is attenuated, the excitation is repeated for multiple times, and response data of each sensor is recorded through the information processing computer;
(5) and processing the data according to the response data of the sensor and the relation between the sensor position direction and the geometric model to obtain the modal parameters of the large-scale structure.
2. The large-scale structure modal testing method according to claim 1, wherein the specific manner of the step (3) is as follows:
(301) establishing a global coordinate system in an information processing computer, and importing a geometric model of a large-scale structure;
(302) determining the position coordinate and the attitude direction of the sensor by utilizing a positioning device and an inclinometer which are arranged in the sensor;
(303) and establishing a relation between the sensor position direction and the large-scale structure geometric model, wherein the relation comprises the specific position of the sensor measuring point in the large-scale structure geometric model and a rotation matrix from a sensor coordinate system to a whole coordinate system.
3. The large-scale structure modal testing method according to claim 1, wherein in the step (4), firstly, the time service function of the positioning device is utilized to perform time synchronization on each sensor; the specific way of applying the step excitation is to excite the large-scale structure in three directions respectively, and at least 10 times of effective free attenuation is recorded in each excitation direction; and after the data recording of each direction is completed, the excitation of the next direction is carried out.
4. The large-scale structural modal testing method according to claim 1, wherein the specific manner of the step (5) is as follows:
(501) obtaining the acceleration response of the sensor under the global coordinate system according to the rotation matrix from the sensor coordinate system to the global coordinate system:
Figure FDA0003405031180000011
in the formula, RnGIs a rotation matrix, vector, from the sensor coordinate system to the global coordinate system
Figure FDA0003405031180000021
For the acceleration response of the sensor in the global coordinate system,
Figure FDA0003405031180000022
the acceleration response of the sensor under the coordinate system of the sensor is obtained;
(502) selecting a sensor as a reference sensor according to the initial natural frequency obtained in the step (1), so that a power spectrogram of the response data of the reference sensor comprises natural frequency components of each order; carrying out Fourier transform on the response data of the reference sensor, wherein each extreme point corresponds to the inherent frequency of different orders;
(503) decomposing response data of the reference sensor to obtain modal responses of all orders, enveloping the modal responses of all orders and carrying out exponential curve fitting to obtain modal damping ratios of different orders; wherein the form of the exponential curve is as follows:
xe=Ae-σt=Ae-2πfξt
in the formula, xeExtracting envelope data on acceleration response, wherein A is a signal amplitude, f is the natural frequency of the order, and xi is a modal damping ratio to be solved;
(504) decomposing the response data of each sensor to obtain concerned modal responses of each order; averaging root mean square values obtained by the same sensors, the same direction, the same order and different excitation orders according to the excitation orders to obtain vibration mode components of the corresponding sensors, the corresponding directions and the corresponding orders; and carrying out maximum value normalization on the vibration mode components of different sensors and the same order to obtain the vibration modes of different orders of the large-scale structure.
CN202111510347.7A 2021-12-10 2021-12-10 Large-scale structure modal testing method Pending CN114383874A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
CN202111510347.7A CN114383874A (en) 2021-12-10 2021-12-10 Large-scale structure modal testing method

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
CN202111510347.7A CN114383874A (en) 2021-12-10 2021-12-10 Large-scale structure modal testing method

Publications (1)

Publication Number Publication Date
CN114383874A true CN114383874A (en) 2022-04-22

Family

ID=81196436

Family Applications (1)

Application Number Title Priority Date Filing Date
CN202111510347.7A Pending CN114383874A (en) 2021-12-10 2021-12-10 Large-scale structure modal testing method

Country Status (1)

Country Link
CN (1) CN114383874A (en)

Citations (6)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN105067213A (en) * 2015-07-16 2015-11-18 北京强度环境研究所 Large-scale structure vibration characteristic test pulse excitation apparatus and application method thereof
CN105424350A (en) * 2015-12-19 2016-03-23 湖南科技大学 Method and system for thin-wall part modal testing based on machine vision
CN107391818A (en) * 2017-07-07 2017-11-24 大连理工大学 A kind of Vibrating modal parameters recognition methods based on state observer
US20190041365A1 (en) * 2017-08-04 2019-02-07 Crystal Instruments Corporation Modal vibration analysis system
CN112771385A (en) * 2018-05-25 2021-05-07 霍廷格布鲁尔及凯尔公司 Method for determining the spatial configuration of a plurality of transducers relative to a target object
CN113155384A (en) * 2020-08-28 2021-07-23 盐城工学院 Sensor arrangement method for reducing uncertainty of structural damping ratio identification

Patent Citations (6)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN105067213A (en) * 2015-07-16 2015-11-18 北京强度环境研究所 Large-scale structure vibration characteristic test pulse excitation apparatus and application method thereof
CN105424350A (en) * 2015-12-19 2016-03-23 湖南科技大学 Method and system for thin-wall part modal testing based on machine vision
CN107391818A (en) * 2017-07-07 2017-11-24 大连理工大学 A kind of Vibrating modal parameters recognition methods based on state observer
US20190041365A1 (en) * 2017-08-04 2019-02-07 Crystal Instruments Corporation Modal vibration analysis system
CN112771385A (en) * 2018-05-25 2021-05-07 霍廷格布鲁尔及凯尔公司 Method for determining the spatial configuration of a plurality of transducers relative to a target object
CN113155384A (en) * 2020-08-28 2021-07-23 盐城工学院 Sensor arrangement method for reducing uncertainty of structural damping ratio identification

Non-Patent Citations (1)

* Cited by examiner, † Cited by third party
Title
静行 等: "随机激励下基于ICA的结构模态参数识别", 噪声与振动控制, no. 06, pages 188 - 193 *

Similar Documents

Publication Publication Date Title
CN107948251B (en) Android-based remote mechanical fault diagnosis system
CN106468623B (en) Powertrain mounting system rigid body mode parameter test method under a kind of whole vehicle state
Koene et al. IoT connected device for vibration analysis and measurement
CN100554884C (en) Method for standardization of optimum 8 positions of flexure gyroscope
CN104897962A (en) Single-frequency signal short sample high precision frequency measurement method and device based on relatively prime perception
CN102279084A (en) Transmission line oscillation positioning system and method based on micro inertial measurement combination
CN101806833A (en) Multi-channel frequency response analysis system and method thereof
JP2012013695A (en) Device for measuring dimensions
CN112710871B (en) Test method and device for positioning speed measurement system host
CN111521141B (en) Device and method for measuring three-dimensional thermal expansion displacement of pipeline
CN103995202B (en) A kind of automatic signal method of testing, Apparatus and system
CN109682562B (en) Multi-axis durability to single-axis durability test method
CN112985867B (en) Steering engine testing method, device, equipment and storage medium
CN114383874A (en) Large-scale structure modal testing method
CN112996107B (en) Antenna device, mobile communication interference signal positioning method and system
CN105510891A (en) In-orbit modal identification method for synthetic aperture radar of satellite
CN109991473B (en) Measuring method and measuring device for current phasor of wire and synchronous phasor measuring device
CN111113486A (en) Performance test method and device of mechanical arm, computer equipment and storage medium
CN113608262B (en) Seismic data processing method and device for calculating rotation component by using translation component
CN111486943B (en) Industrial robot vibration state analysis method, system and device and readable storage medium
CN112966346B (en) Frequency response function uncertainty analysis method based on equivalent frequency dispersion
CN114839482A (en) Power frequency withstand voltage breakdown position positioning method and device of low-voltage comprehensive distribution box
CN205015079U (en) Little wind vibration of transmission line moves monitoring devices
CN109631809B (en) Bridge deflection measuring equipment and method
CN109238369A (en) A kind of stress and strain testing method based on MEMS sensor

Legal Events

Date Code Title Description
PB01 Publication
PB01 Publication
SE01 Entry into force of request for substantive examination
SE01 Entry into force of request for substantive examination