GB/T 11349.2-2025 English PDFUS$564.00 · In stock
Delivery: <= 5 days. True-PDF full-copy in English will be manually translated and delivered via email. GB/T 11349.2-2025: Mechanical vibration and shock - Experimental determination of mechanical mobility - Part 2: Measurements using single-point translation excitation with an attached vibration exciter Status: Valid GB/T 11349.2: Historical versions
Basic dataStandard ID: GB/T 11349.2-2025 (GB/T11349.2-2025)Description (Translated English): Mechanical vibration and shock - Experimental determination of mechanical mobility - Part 2: Measurements using single-point translation excitation with an attached vibration exciter Sector / Industry: National Standard (Recommended) Classification of Chinese Standard: J04 Classification of International Standard: 17.160 Word Count Estimation: 28,258 Date of Issue: 2025-06-30 Date of Implementation: 2026-01-01 Older Standard (superseded by this standard): GB/T 11349.2-2006 Issuing agency(ies): State Administration for Market Regulation, China National Standardization Administration GB/T 11349.2-2025: Mechanical vibration and shock - Experimental determination of mechanical mobility - Part 2: Measurements using single-point translation excitation with an attached vibration exciter---This is an excerpt. Full copy of true-PDF in English version (including equations, symbols, images, flow-chart, tables, and figures etc.), auto-downloaded/delivered in 9 seconds, can be purchased online: https://www.ChineseStandard.net/PDF.aspx/GBT11349.2-2025 ICS 17.160 CCSJ04 National Standard of the People's Republic of China Replaces GB/T 11349.2-2006 Experimental determination of mechanical vibration and shock admittance Part 2.Single-point translational excitation measurements using a shaker (ISO 7626-2.2015, IDT) Released on June 30, 2025 Implementation on January 1, 2026 State Administration for Market Regulation The National Standardization Administration issued Table of ContentsPreface III Introduction IV 1 Scope 1 2 Normative references 1 3 Terms and Definitions 1 4 Overall structure of the measurement system 2 5 Support of test structure 3 6 Inspiration 4 7 Measurement of Excitation Force and Its Motion Response 9 8 Sensor signal processing 11 9 Control of Incentives 12 10 Verification of valid data 16 11 Modal Parameter Identification 16 Appendix A (Normative) Validity Test of Measurement Results 17 Appendix B (Normative) Requirements for Excitation Frequency Increment and Duration 20 Appendix C (Informative) Modal Parameter Identification 21 Reference 22 Preface This document is in accordance with the provisions of GB/T 1.1-2020 "Guidelines for standardization work Part 1.Structure and drafting rules for standardization documents" Drafting. This document is Part 2 of GB/T 11349 "Mechanical vibration and shock - Test determination of mechanical admittance". GB/T 11349 has been The following parts were published. --- Part 1.Basic terms and definitions, sensor characteristics; --- Part 2.Measurement of single-point translational excitation using a vibrator; --- Part 3.Impact excitation method. This document replaces GB/T 11349.2-2006 "Test determination of mechanical admittance for vibration and shock - Part 2.Using a single exciter Compared with GB/T 11349.2-2006, in addition to structural adjustments and editorial changes, the main technical changes are as follows. --- Changed the overview of incentives (see 6.1, 6.1 of the.2006 edition); --- Added an overview of other stimulus waveforms (see 6.2.5); --- Added "rotating eccentric mass exciter" (see 6.3); --- Change "Note 1 to Note 4 in 7.3" to the main text, and change "When the ratio of effective mass is greater than 0.06 and less than 0.5, The mass reduction method should be used when the effective mass ratio is greater than 0.05 and less than 0.5. (See 7.3, 7.3 of the.2006 edition); --- Added the requirement that "the sampling frequency should be at least ten times higher than the frequency of interest" (see 8.4.1). This document is equivalent to ISO 7626-2.2015 "Mechanical vibration and shock - Test determination of mechanical admittance - Part 2.Tests using a vibrator" Single-point translational excitation measurement". Please note that some of the contents of this document may involve patents. The issuing organization of this document does not assume the responsibility for identifying patents. This document was drafted by. China Machinery Engineering Corporation Zhengzhou Machinery Research Institute Co., Ltd., Northwest Mechanical and Electrical Engineering Research Institute, Huadian Electric Power Science and Technology Co., Ltd. China Academy of Sciences Co., Ltd., Guangdong New Energy Storage National Research Institute Co., Ltd., North China University of Technology, State Grid Hubei Electric Power Co., Ltd. Science Research Institute, Dongguan Guangbo Laser Technology Co., Ltd., Huaxia High-speed Railway Technology Co., Ltd., Beijing Machinery Industry Automation Research Institute Co., Ltd. and Henan Jiuyu Enpai Electric Power Technology Co., Ltd. The main drafters of this document are. Ma Weiping, Chao Hongxiao, Bing Hankun, Yang Yi, Yan Yu, Wang Yanjie, Dou Lisha, Huang Haizhou, Zhou Miao, Liu Wen, Xu Haiyong, Zhu Xiaomin, and Zhang Yingshuai. This document was first issued in 1989, revised for the first time in.2006, and this is the second revision.introduction0.1 Comprehensive Introduction to ISO 7626 for Admittance Measurement The dynamic characteristics of the structure can be determined by the relevant frequency response function obtained from the admittance measurement, or by the acceleration corresponding to the frequency response function. Each frequency response function is the motion response at a point in the structure due to unit force or moment excitation. The magnitude and phase of these functions are functions of frequency. The difference between acceleration admittance, displacement admittance and admittance is that acceleration or displacement is used instead of velocity to represent the motion response. For the sake of simplicity, only the term "admittance" will be used in the various parts of ISO 7626.Of course, all test methods and requirements apply to accelerated Determination of degree admittance and displacement admittance. Typical applications of admittance measurement. a) predict the dynamic response of a structure to known or assumed input excitations; b) Determine the modal characteristics of the structure (natural frequency, damping ratio and mode shape); c) predicting dynamic interactions between connected structures; d) verify the validity of the mathematical model of the structure and improve its accuracy; e) Determine the dynamic properties (i.e., complex elastic modulus) of single or composite materials. In some applications, it may be necessary to measure forces and motions along three mutually perpendicular axes, as well as moments and rotations around these three axes. To fully describe the dynamic characteristics. For each point of interest, these measurements give a 6×6 admittance matrix. point, the system has an overall admittance matrix of size (6N×6N). In most practical applications, it is not necessary to know the entire (6N×6N) matrix. Usually, only a single point and a single direction of excitation are required. It is sufficient to measure the admittance of the driving point and some transfer admittance by measuring the translation response at the key points of the structure. In this case, only the rotational admittance may be of interest. Mechanical admittance is defined as the frequency-dependent ratio of the phasor of the translational or rotational velocity response to the phasor of the applied exciting force or torque. If the response is measured with an accelerometer, it must be converted to velocity to obtain admittance. Alternatively, the acceleration and force The ratio of force, i.e. acceleration, can be used to characterize the structure. In other cases, the displacement admittance, i.e. the ratio of displacement to force, can be used. NOTE. Conventionally, the frequency response function of a structure is usually expressed as the reciprocal of one of the above dynamic characteristics. The arithmetic reciprocal of the mechanical admittance is often called the mechanical impedance. However, note that this is a misconception, as the arithmetic reciprocal of admittance does not usually represent any element of the impedance matrix of a structure. Instead, admittance is converted to Impedance requires the inversion of the admittance matrix. This is described in detail in ISO 7626-1. Admittance test data cannot be used directly as part of the structural impedance model. To make the data compatible with the model, the impedance matrix of the model is Convert to an admittance matrix and vice versa (for restrictions see ISO 7626-1). 0.2 Introduction to this document In many applications of mechanical admittance data, the structure is excited at a certain position and direction, and the translational response is measured at some key points to determine the correct mechanical admittance data. The admittance of the fixed driving point and a small amount of transfer admittance are sufficient. These translational excitation forces can be applied by means of a shaker connected to the test structure or by means of a The device is attached to the structure. Classifying the actuation devices as "connected" and "unconnected" makes a significant difference in the ease with which the actuation point can be moved to a new location. For example, when using a vibrating hammer, it is easier to change the pulse application location than to move a connected vibrator to a new location on the structure. Both excitation methods have their own applications for which they are best suited. This document deals with measurements using a single connected shaker; ISO 7626- 5.Applicable to shock excitation measurements without a connected shaker. 0.3 About the composition of GB/T 11349 GB/T 11349 "Mechanical vibration and shock - Test determination of mechanical admittance" mainly stipulates the mechanical system under vibration and shock conditions. Test methods for determining mechanical admittance, including term definitions, test principles, equipment requirements, test procedures, data processing, and test reports. It is suitable for the dynamic characteristics analysis of mechanical structures, equipment and their components, and aims to provide a scientific basis for the vibration and impact characteristics analysis of mechanical systems. GB/T 11349 is intended to consist of three parts. --- Part 1.Basic terms and definitions, sensor characteristics. The purpose is to define basic terms and specify the Calibration tests, environmental tests and physical measurements required to verify the suitability of impedance probes, force sensors and motion response sensors The method mainly provides guidance for the selection, calibration and evaluation of sensors and measuring instruments suitable for mechanical admittance measurement. --- Part 2.Single-point translational excitation measurement using a vibrator. The purpose is to specify the single-point translational excitation measurement connected to the structure under test. A method for measuring the mechanical admittance and other frequency response functions of structures (such as buildings, machines and vehicles) using a vibrator. --- Part 3.Impact excitation method. The purpose is to specify how to use an impact exciter that is not connected to the structure to excite the structure to measure Methods for its mechanical admittance and other frequency response functions. Experimental determination of mechanical vibration and shock admittance Part 2.Single-point translational excitation measurements using a shaker 1 Scope This document specifies the method for measuring the linear mechanical admittance and Other frequency response function methods. This document applies to measurements of admittance, acceleration, or displacement, whether driven-point or transfer measurements. It also applies to the determination of these Although a single point excitation is used, there is no limit to the number of motion responses that can be measured simultaneously. For example, multi-point response measurements required in modal analysis. 2 Normative references The contents of the following documents constitute the essential clauses of this document through normative references in this document. For referenced documents without a date, only the version corresponding to that date applies to this document; for referenced documents without a date, the latest version (including all amendments) applies to This document. ring-Vocabulary) Note. GB/T 2298-2010 Mechanical vibration, shock and condition monitoring vocabulary (ISO 2041.2009, IDT) ISO 7626-1 Mechanical vibration and shock — Test determination of mechanical admittance — Part 1.Basic terms and definitions, sensor characteristics Note. GB/T 11349.1-2018 Mechanical vibration and shock - Test determination of mechanical admittance - Part 1.Basic terms and definitions, sensor characteristics (ISO 7626-1.2011, IDT) 3 Terms and Definitions For the purposes of this document, the terms and definitions defined in ISO 2041 and ISO 7626-1 and the following apply. NOTE. As this document deals with mechanical admittance, the following definition notes provide more detail than in ISO 2041. 3.1 frequency-responsefunction The ratio of the complex motion response of a frequency-dependent linear system to the complex excitation force. NOTE 1 The stimulus is a simple harmonic, random or transient function of time. If the test structure is considered as a linear system within a certain stimulus or response range, the frequency response The response function no longer depends on the type of stimulus function. In this case, the test results obtained under one stimulus are used to predict the system's response to the other stimulus. The phasors and their equivalents for random and transient excitations are discussed in Appendix B. Note 2.In fact, the linearity of the system is conditional and can only be approximately satisfied. The linearity of the system depends on the type of system and the size of the input. Be careful to avoid nonlinear The effects of nonlinearity are not observed, especially when pulse excitation is used. Tests are conducted without pulse excitation on structures known to be nonlinear (e.g. some riveted structures) and And you need to be extra careful when using random excitation tests on such structures. Note 3.Motion is expressed in terms of velocity, acceleration, and displacement, and the corresponding frequency response functions are called admittance (sometimes called mechanical admittance), acceleration admittance (sometimes called It is also mistakenly called "inertia". Avoid using it because it conflicts with the common definition of "acoustic inertia" and also contradicts the definition of the term "inertia". The term "inertia" is used to describe the properties of the material (e.g., moment of inertia) and displacement admittance (sometimes called dynamic compliance). ......Tips & Frequently Asked Questions:Question 1: How long will the true-PDF of GB/T 11349.2-2025_English be delivered?Answer: Upon your order, we will start to translate GB/T 11349.2-2025_English as soon as possible, and keep you informed of the progress. The lead time is typically 3 ~ 5 working days. The lengthier the document the longer the lead time.Question 2: Can I share the purchased PDF of GB/T 11349.2-2025_English with my colleagues?Answer: Yes. 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