CN114324979A - Accelerometer vibration detuning error evaluation method and device, storage medium and equipment - Google Patents

Accelerometer vibration detuning error evaluation method and device, storage medium and equipment Download PDF

Info

Publication number
CN114324979A
CN114324979A CN202210007318.7A CN202210007318A CN114324979A CN 114324979 A CN114324979 A CN 114324979A CN 202210007318 A CN202210007318 A CN 202210007318A CN 114324979 A CN114324979 A CN 114324979A
Authority
CN
China
Prior art keywords
accelerometer
vibration
normal distribution
establishing
output
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
CN202210007318.7A
Other languages
Chinese (zh)
Other versions
CN114324979B (en
Inventor
张国兵
段磊强
钟秀峰
宋文强
高阳
宋俊霞
戴居峰
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.)
Beijing Sunwise Space Technology Ltd
Original Assignee
Beijing Sunwise Space Technology Ltd
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 Beijing Sunwise Space Technology Ltd filed Critical Beijing Sunwise Space Technology Ltd
Priority to CN202210007318.7A priority Critical patent/CN114324979B/en
Publication of CN114324979A publication Critical patent/CN114324979A/en
Application granted granted Critical
Publication of CN114324979B publication Critical patent/CN114324979B/en
Active legal-status Critical Current
Anticipated expiration legal-status Critical

Links

Images

Abstract

The invention discloses an accelerometer vibration maladjustment error evaluation method, an accelerometer vibration maladjustment error evaluation device, a storage medium and equipment, wherein the evaluation method comprises the following steps: (1) establishing accelerometer input excitation based on a random vibration principle; (2) establishing an accelerometer vibration output model, and modeling accelerometer output into a truncated normal distribution; (3) and (3) deducing the expectation of the truncated normal distribution according to the steps (1) and (2) and calculating the vibration imbalance error of the accelerometer. The evaluation device includes: an input excitation establishing module is used for establishing accelerometer input excitation based on a random vibration principle; the output model establishing module is used for establishing an accelerometer vibration output model and establishing an accelerometer output model as a truncation type normal distribution; and the calculation module is used for calculating the vibration imbalance error of the accelerometer according to the expectation of the derivation truncation type normal distribution. The evaluation method can effectively reduce the design risk of the inertial navigation system, shorten the development time and improve the reliability of the inertial navigation system.

Description

Accelerometer vibration detuning error evaluation method and device, storage medium and equipment
Technical Field
The invention relates to the technical field of accelerometers, in particular to an accelerometer vibration imbalance error evaluation method, device, storage medium and equipment.
Background
The aircraft is influenced by atmospheric fluctuation, self engine vibration and the like in the flying process, the attitude stability of the aircraft is ensured, and the inertial navigation system is ensured not to be interfered by the vibration signals and to output effective attitude information. The accelerometer is used as a main device for measuring the inertial navigation of the aircraft, is sensitive to vibration information, and the output precision of the accelerometer directly influences the precision of an inertial navigation system.
The conventional technical scheme is that after the design of an inertial navigation system is finished, the flying application working condition of an aircraft is simulated through a vibrating table to verify the performance index of the inertial navigation system.
Disclosure of Invention
In order to solve the defects of the prior art, the invention provides an accelerometer vibration imbalance error evaluation method, an accelerometer vibration imbalance error evaluation device, a storage medium and an accelerometer vibration model.
In order to realize the purpose of the invention, the following scheme is adopted:
an accelerometer vibration detuning error assessment method comprises the following steps:
(1) establishing accelerometer input excitation based on a random vibration principle;
(2) establishing an accelerometer vibration output model, and modeling accelerometer output into a truncated normal distribution;
(3) and (3) deducing the expectation of the truncated normal distribution according to the steps (1) and (2) and calculating the vibration imbalance error of the accelerometer.
Further, in the step (1), the random vibration signals generated in the external vibration process generally follow a Gaussian distribution X-N (mu, delta)2) The accelerometer tests were all performed under a 1g gravity field.
Further, in the step (2), the output of the accelerometer follows normal distribution X-N (mu, delta)2) The probability density function is expressed as:
Figure BDA0003457480510000021
taking a truncation interval (a, b), wherein a is the minimum value of the output range of the accelerometer, b is the maximum value of the output range of the accelerometer, and expressing the probability density function of X by a standard normal distribution probability density function and a cumulative distribution function through a standardized variable:
Figure BDA0003457480510000022
where Φ (t) is the standard normal distribution cumulative distribution function:
Figure BDA0003457480510000023
phi (t) is a standard normal distribution probability density function:
Figure BDA0003457480510000024
further, in step (3), the expectation of the truncated normal distribution is derived from steps (1) and (2):
Figure BDA0003457480510000031
substituting equation (1) into equation (2):
Figure BDA0003457480510000032
further, under random vibration, the mean value μ' of the vibration detuning error of the accelerometer is:
Figure BDA0003457480510000033
wherein mu is 1g under a gravity field, delta is a random vibration signal input root mean square, and a and b are accelerometer measuring ranges.
An accelerometer vibration misalignment error assessment apparatus comprising:
establishing an input excitation module for establishing accelerometer input excitation based on a random vibration principle, wherein accelerometer tests are carried out in a 1g gravity field;
the output model establishing module is used for establishing an accelerometer vibration output model and establishing an accelerometer output model as a truncation type normal distribution;
and the calculation module is used for calculating the vibration imbalance error of the accelerometer according to the expectation of the derivation truncation type normal distribution.
Furthermore, when the output model building module builds the output model, the output of the accelerometer follows normal distribution X-N (mu, delta)2) The probability density function is expressed as:
Figure BDA0003457480510000041
taking a truncation interval (a, b), wherein a is the minimum value of the output range of the accelerometer, b is the maximum value of the output range of the accelerometer, and expressing the probability density function of X by a standard normal distribution probability density function and a cumulative distribution function through a standardized variable:
Figure BDA0003457480510000042
where Φ (t) is the standard normal distribution cumulative distribution function:
Figure BDA0003457480510000043
phi (t) is a standard normal distribution probability density function:
Figure BDA0003457480510000044
further, the calculation module derives an expectation of a truncated normal distribution:
Figure BDA0003457480510000051
substituting equation (1) into equation (2):
Figure BDA0003457480510000052
further, under random vibration, when the calculation module calculates the accelerometer vibration imbalance error, the accelerometer vibration imbalance error mean value μ' is:
Figure BDA0003457480510000053
wherein mu is 1g under a gravity field, delta is a random vibration signal input root mean square, and a and b are accelerometer measuring ranges.
A computer-readable storage medium having stored thereon a computer program which, when executed by a processor, controls a storage medium device to perform the accelerometer vibration misalignment error assessment method described above.
An electronic device, comprising: at least one processor and memory; the memory stores computer-executable instructions, and the at least one processor executes the computer-executable instructions stored in the memory, so that the at least one processor executes the accelerometer vibration imbalance error assessment method.
The invention has the beneficial effects that: aiming at an alternating current signal generated by external vibration in the application of an inertial navigation system, an evaluation method is provided for the imbalance error of an accelerometer in a vibration environment, and the evaluation method can effectively reduce the design risk of the inertial navigation system, shorten the development time and improve the reliability of the inertial navigation system; the evaluation method is small in required calculation amount, simple and easy to implement, low in implementation cost, beneficial to improvement of offset error evaluation under accelerometer vibration, beneficial to improvement of direct current offset performance of accelerometer products in high-precision measurement, and good in practical value.
Drawings
FIG. 1 shows the random vibration acceptance test requirements of a certain integrated navigation product in an embodiment;
FIG. 2 is a random vibration sampling level test requirement of a certain integrated navigation product in an embodiment;
FIG. 3 is an error curve of accelerometer vibration imbalance under the condition of FIG. 1 for a certain integrated navigation product in an embodiment;
FIG. 4 is a graph of the accelerometer vibration detuning error under the condition of FIG. 2 for a certain integrated navigation product in an embodiment;
FIG. 5 is a vibration detuning error curve of an accelerometer of an integrated navigation product according to an embodiment after the accelerometer has modified range under the condition of FIG. 2;
FIG. 6 is a flowchart of an evaluation method in an embodiment.
Detailed Description
Example 1
As shown in fig. 6, the present embodiment provides an accelerometer vibration detuning error evaluation method, including the following steps:
(1) establishing accelerometer input excitation based on a random vibration principle;
the random vibration signal is a non-deterministic signal that cannot be described by a deterministic mathematical relationship, but only by statistical methods. Accurate values cannot be predicted at any instant in the future, and any observed value only represents a result which can be generated in the variation range of the observed value, but the variation of the observed value is subject to a statistical rule. A given random spectrogram contains all information of the random signal, including the frequency range of the random vibration, the energy value of each frequency of the random vibration and the root mean square of the random vibration acceleration. The performance of the accelerometer in most application scenarios can be measured by random vibration.
The random vibration signal generally follows Gaussian distribution X-N (mu, delta)2) Wherein, mu, delta2For normal distribution random variable mathematical expectation and variance, accelerometer tests are all performed under a 1g gravity field, X-N (mu, delta)2) Obeying a gaussian distribution, the random variable Y ═ X +1 similarly obeys a gaussian distribution, Y to N (μ +1, δ)2)。
(2) Establishing an accelerometer vibration output model, and modeling accelerometer output into a truncated normal distribution;
in the step (2), the accelerometer senses an input signal, the output of the accelerometer is consistent with the input and also obeys Gaussian distribution, but the output of the accelerometer is modeled into a cut-off normal distribution because the accelerometer has a measuring range, and the output of the accelerometer obeys normal distribution X-N (mu, delta)2) The probability density function is expressed as:
Figure BDA0003457480510000071
taking a truncation interval (a, b), wherein a is the minimum value of the output range of the accelerometer, b is the maximum value of the output range of the accelerometer, and expressing the probability density function of X by a standard normal distribution probability density function and a cumulative distribution function through a standardized variable:
Figure BDA0003457480510000081
where Φ (t) is the standard normal distribution cumulative distribution function:
Figure BDA0003457480510000082
phi (t) is a standard normal distribution probability density function:
Figure BDA0003457480510000083
(3) deducing expectation of the truncated normal distribution according to the steps (1) and (2), and calculating the vibration imbalance error of the accelerometer;
in step (3), the expectation of the truncated normal distribution is deduced from steps (1) and (2):
Figure BDA0003457480510000084
substituting equation (1) into equation (2):
Figure BDA0003457480510000085
under random vibration, the mean value μ' of the vibration detuning error of the accelerometer is:
Figure BDA0003457480510000091
wherein mu is 1g under a gravity field, delta is a random vibration signal input root mean square, and a and b are accelerometer measuring ranges.
Specific examples of the present invention are described in further detail below.
For example, in a combined navigation product, the random vibration power spectral density of the combined navigation product is as shown in fig. 1 and 2, the accelerometer has a range of ± 30g, and under the vibration condition of fig. 1 and 2, the accelerometer parallel to the gravity field works for 50s, and the error offset is less than 20 m.
The method comprises the following specific steps:
(1) establishing accelerometer input excitation based on a random vibration principle, wherein the root mean square of random vibration is calculated to be mu-1 and delta-7.67 as shown in fig. 1;
(2) establishing an accelerometer vibration output model, wherein the accelerometer output follows normal distribution X-N (mu, delta)2) The truncation interval (-30,30) is the accelerometer with the measuring range of +/-30 g;
(3) calculating the vibration maladjustment error of the accelerometer, and substituting the data in the steps (1) and (2)
Figure BDA0003457480510000092
The accelerometer vibration detuning error mu' is related to the random vibration input root mean square curve as shown in FIG. 3. As can be seen from FIG. 3, under the condition of FIG. 1, the vibration detuning error of the accelerometer is 0.001539g, and the displacement deviation thereof is less than 2m, so as to meet the task requirement. Repeating steps (1), (2) and (3) under the conditions of fig. 2, wherein the root mean square of the random oscillations in step (1) is calculated as μ ═ 1, δ ═ 18.34; the accelerometer vibration detuning error mu' is related to the random vibration input root mean square curve as shown in FIG. 4. As can be seen from FIG. 4, under the condition of FIG. 2, the vibration detuning error of the accelerometer is 0.3813g, the displacement deviation thereof is much larger than 20m, and the task requirement cannot be met, and the random vibration test is performed on the actual product under the condition, and the calculation result of FIG. 4 is verified.
Repeating steps (1), (2) and (3) under the conditions of fig. 2, wherein the root mean square of the random oscillations in step (1) is calculated as μ ═ 1, δ ═ 18.34; step (2) accelerometer vibration output model establishment, wherein accelerometer output obeys normal distribution X-N (1, 18.34)2) The truncation interval (-60,60) is the accelerometer with the measuring range of +/-60 g; the accelerometer vibration detuning error mu' is plotted against the random vibration input root mean square curve in FIG. 5. As can be seen from FIG. 5, under the condition of FIG. 2, the vibration offset error of the accelerometer is 0.01245g, and the displacement deviation is less than 20m, so that the task requirement can be met, and the calculation result of FIG. 5 is verified by performing a random vibration test on an actual product under the condition.
As can be seen from fig. 3, 4 and 5, under the same input vibration condition, the larger the accelerometer range is, the smaller the vibration detuning error μ' is; the larger the root mean square value of the certain input vibration condition of the accelerometer range is, the larger the vibration detuning error mu' of the accelerometer is.
The error evaluation method of the embodiment is small in required calculated amount, simple and easy to implement, low in implementation cost, not only beneficial to improvement of imbalance error evaluation under accelerometer vibration, but also beneficial to improvement of direct current offset performance of accelerometer products in high-precision measurement, and good in practical value.
Example 2
The embodiment provides another accelerometer vibration detuning error evaluation device, which comprises:
establishing an input excitation module for establishing accelerometer input excitation based on a random vibration principle, wherein accelerometer tests are carried out in a 1g gravity field;
the output model establishing module is used for establishing an accelerometer vibration output model and establishing an accelerometer output model as a truncation type normal distribution;
the output of the accelerometer follows normal distribution X-N (mu, delta)2) The probability density function is expressed as:
Figure BDA0003457480510000111
taking a truncation interval (a, b), wherein a is the minimum value of the output range of the accelerometer, b is the maximum value of the output range of the accelerometer, and expressing the probability density function of X by a standard normal distribution probability density function and a cumulative distribution function through a standardized variable:
Figure BDA0003457480510000112
where Φ (t) is the standard normal distribution cumulative distribution function:
Figure BDA0003457480510000113
phi (t) is a standard normal distribution probability density function:
Figure BDA0003457480510000114
the calculation module is used for calculating the vibration detuning error of the accelerometer according to the expectation of the derivation truncation type normal distribution;
when deriving the expectation of a truncated normal distribution:
Figure BDA0003457480510000121
substituting equation (1) into equation (2):
Figure BDA0003457480510000122
under random vibration, when the calculation module calculates the accelerometer vibration maladjustment error, the accelerometer vibration maladjustment error mean value mu' is:
Figure BDA0003457480510000123
wherein mu is 1g under a gravity field, delta is a random vibration signal input root mean square, and a and b are accelerometer measuring ranges.
Example 3
The present embodiment provides a computer-readable storage medium having stored thereon a computer program which, when executed by a processor, controls a storage medium device to execute the accelerometer vibration imbalance error assessment method of embodiment 1.
Example 4
The embodiment provides an electronic device, including: at least one processor and memory; wherein the memory stores computer-executable instructions, and the computer-executable instructions stored in the memory are executed on the at least one processor to cause the at least one processor to perform the accelerometer vibration imbalance error assessment method of embodiment 1.
The above embodiments are only for illustrating the technical ideas and features of the present invention, and are not meant to be exclusive or limiting of the present invention. It will be understood by those skilled in the art that various changes may be made and equivalents may be substituted without departing from the scope of the invention.

Claims (10)

1. An accelerometer vibration imbalance error assessment method is characterized by comprising the following steps:
(1) establishing accelerometer input excitation based on a random vibration principle;
(2) establishing an accelerometer vibration output model, and modeling accelerometer output into a truncated normal distribution;
(3) and (3) deducing the expectation of the truncated normal distribution according to the steps (1) and (2) and calculating the vibration imbalance error of the accelerometer.
2. The method for evaluating the vibration detuning error of the accelerometer according to claim 1, wherein in the step (1), the random vibration signals generated in the external vibration process generally follow a Gaussian distribution X-N (mu, delta)2) The accelerometer tests were all performed under a 1g gravity field.
3. The method of claim 2, wherein in step (2), the accelerometer output follows a normal distribution X-N (μ, δ)2) The probability density function is expressed as:
Figure FDA0003457480500000011
taking a truncation interval (a, b), wherein a is the minimum value of the output range of the accelerometer, b is the maximum value of the output range of the accelerometer, and expressing the probability density function of X by a standard normal distribution probability density function and a cumulative distribution function through a standardized variable:
Figure FDA0003457480500000012
where Φ (t) is the standard normal distribution cumulative distribution function:
Figure FDA0003457480500000021
phi (t) is a standard normal distribution probability density function:
Figure FDA0003457480500000022
4. the method according to claim 3, wherein in step (3), the expectation of the truncated normal distribution is derived from steps (1) and (2):
Figure FDA0003457480500000023
substituting equation (1) into equation (2):
Figure FDA0003457480500000024
5. the method of claim 4, wherein the mean value μ' of the vibration imbalance errors of the accelerometer under random vibration is:
Figure FDA0003457480500000025
wherein mu is 1g under a gravity field, delta is a random vibration signal input root mean square, and a and b are accelerometer measuring ranges.
6. An accelerometer vibration imbalance error assessment apparatus, comprising:
establishing an input excitation module for establishing accelerometer input excitation based on a random vibration principle, wherein accelerometer tests are carried out in a 1g gravity field;
the output model establishing module is used for establishing an accelerometer vibration output model and establishing an accelerometer output model as a truncation type normal distribution;
and the calculation module is used for calculating the vibration imbalance error of the accelerometer according to the expectation of the derivation truncation type normal distribution.
7. The apparatus of claim 6, wherein the output model building module builds the output model such that the accelerometer output follows a normal distribution X-N (μ, δ) when the accelerometer output is modeled2) The probability density function is expressed as:
Figure FDA0003457480500000031
taking a truncation interval (a, b), wherein a is the minimum value of the output range of the accelerometer, b is the maximum value of the output range of the accelerometer, and expressing the probability density function of X by a standard normal distribution probability density function and a cumulative distribution function through a standardized variable:
Figure FDA0003457480500000032
where Φ (t) is the standard normal distribution cumulative distribution function:
Figure FDA0003457480500000033
phi (t) is a standard normal distribution probability density function:
Figure FDA0003457480500000041
8. the accelerometer vibration imbalance error assessment device of claim 8, wherein the calculation module derives the expected time of the truncated normal distribution:
Figure FDA0003457480500000042
substituting equation (1) into equation (2):
Figure FDA0003457480500000043
9. a computer-readable storage medium having a computer program stored thereon, wherein the computer program, when executed by a processor, controls a storage medium device to perform the accelerometer vibration misalignment error assessment method of any of claims 1-5.
10. An electronic device, comprising: at least one processor and memory; wherein the memory stores computer-executable instructions, wherein execution of the computer-executable instructions stored in the memory on the at least one processor causes the at least one processor to perform the accelerometer vibration imbalance error assessment method of any one of claims 1 to 5.
CN202210007318.7A 2022-01-06 2022-01-06 Accelerometer vibration imbalance error assessment method, accelerometer vibration imbalance error assessment device, storage medium and accelerometer vibration imbalance error assessment device Active CN114324979B (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
CN202210007318.7A CN114324979B (en) 2022-01-06 2022-01-06 Accelerometer vibration imbalance error assessment method, accelerometer vibration imbalance error assessment device, storage medium and accelerometer vibration imbalance error assessment device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
CN202210007318.7A CN114324979B (en) 2022-01-06 2022-01-06 Accelerometer vibration imbalance error assessment method, accelerometer vibration imbalance error assessment device, storage medium and accelerometer vibration imbalance error assessment device

Publications (2)

Publication Number Publication Date
CN114324979A true CN114324979A (en) 2022-04-12
CN114324979B CN114324979B (en) 2024-04-02

Family

ID=81024605

Family Applications (1)

Application Number Title Priority Date Filing Date
CN202210007318.7A Active CN114324979B (en) 2022-01-06 2022-01-06 Accelerometer vibration imbalance error assessment method, accelerometer vibration imbalance error assessment device, storage medium and accelerometer vibration imbalance error assessment device

Country Status (1)

Country Link
CN (1) CN114324979B (en)

Citations (7)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN101819216A (en) * 2010-05-06 2010-09-01 哈尔滨工业大学 Testing device for orthogonal double high-precision accelerometers
CN101929888A (en) * 2009-06-23 2010-12-29 株式会社山武 Amplitude computing apparatus and method
CN106844836A (en) * 2016-10-19 2017-06-13 北京航空航天大学 A kind of quartz flexible accelerometer parametric stability modeling method
CN109827571A (en) * 2019-03-22 2019-05-31 北京壹氢科技有限公司 A kind of dual acceleration meter calibration method under the conditions of no turntable
CN111289773A (en) * 2018-12-06 2020-06-16 航天科工惯性技术有限公司 Accelerometer vibration rectification error test device and method
CN112818601A (en) * 2021-02-05 2021-05-18 河海大学 Hydroelectric generating set health assessment method based on GA-BP neural network and error statistical analysis
CN113239558A (en) * 2021-05-21 2021-08-10 中国工程物理研究院总体工程研究所 Mechanism and data combined driving transportation vibration modeling method

Patent Citations (7)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN101929888A (en) * 2009-06-23 2010-12-29 株式会社山武 Amplitude computing apparatus and method
CN101819216A (en) * 2010-05-06 2010-09-01 哈尔滨工业大学 Testing device for orthogonal double high-precision accelerometers
CN106844836A (en) * 2016-10-19 2017-06-13 北京航空航天大学 A kind of quartz flexible accelerometer parametric stability modeling method
CN111289773A (en) * 2018-12-06 2020-06-16 航天科工惯性技术有限公司 Accelerometer vibration rectification error test device and method
CN109827571A (en) * 2019-03-22 2019-05-31 北京壹氢科技有限公司 A kind of dual acceleration meter calibration method under the conditions of no turntable
CN112818601A (en) * 2021-02-05 2021-05-18 河海大学 Hydroelectric generating set health assessment method based on GA-BP neural network and error statistical analysis
CN113239558A (en) * 2021-05-21 2021-08-10 中国工程物理研究院总体工程研究所 Mechanism and data combined driving transportation vibration modeling method

Non-Patent Citations (1)

* Cited by examiner, † Cited by third party
Title
LONG PHAM 等: "MEMS加速度计的振动校正", 今日电子, 31 July 2017 (2017-07-31), pages 20 - 22 *

Also Published As

Publication number Publication date
CN114324979B (en) 2024-04-02

Similar Documents

Publication Publication Date Title
CN102436515A (en) Methods and systems for assessing residual life of turbomachine airfoils
CN109459061A (en) Micro inertial measurement unit scaling method, equipment and computer readable storage medium
US20140303907A1 (en) Systems and methods for dynamic force measurement
CN110736400B (en) Underwater drilling blasting vibration velocity calculation method considering internal rock structure
CN106468554A (en) A kind of measuring method of the contactless inertial parameter of rolling satellite
CN109556765A (en) A kind of blade non-contacting vibration strain measurements conversion method
KR20110085495A (en) Method for calibrating sensor errors automatically during operation, and inertial navigation using the same
US20150073730A1 (en) Mechanical strain gauge simulation
Cruciat et al. Experimental determination of dynamic characteristics of structures
CN114324979A (en) Accelerometer vibration detuning error evaluation method and device, storage medium and equipment
CN113188716A (en) Dynamic calibration method and device and stability verification method and device for force sensor
CN102538824B (en) Method suitable for MEMS IMU repeated multiple calibrating
CN115790665A (en) Gyro error compensation method and device, electronic equipment and storage medium
Abhinav et al. Improvements in the sensitivity of mems based gyroscope for military applications
CN114912329A (en) Modeling method and device of battery pack model, electronic equipment and storage medium
CN110987018A (en) Method and system for calibrating DVL (dynamic Voltage laser) error by using position method of specific force differential
Farago et al. Experimental study on free vibratory behavior of nonlinear structure
CN110260888A (en) A kind of swing angle measuring method, apparatus and system
Chi et al. Research on the FMECA and Random Vibration Test for Micro Inertial Measurement Unit
CN115164888B (en) Error correction method and device, electronic equipment and storage medium
KR101130069B1 (en) Methode for calculating angular velocity using trapping measurment of ring laser gyroscope
CN116295389B (en) Method, device, equipment and medium for stably switching strapdown compass system state
Lechner Techniques for the development of error models for aided strapdown navigation systems
Murphy et al. Efficient Unsteady Model Estimation Using Computational and Experimental Data
Xing et al. A System-Level Simulation Approach for Analyzing MEMS Gyroscope Manufacture Error

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
GR01 Patent grant
GR01 Patent grant