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1、INTERNATIONAL STANDARD ISO 16063-13 First edition 2001-12-01 Reference number ISO 16063-13:2001(E) ISO 2001 Methods for the calibration of vibration and shock transducers Part 13: Primary shock calibration using laser interferometry Mthodes pour ltalonnage des transducteurs de vibrations et de chocs
2、 Partie 13: talonnage primaire de chocs par interfromtrie laser Copyright International Organization for Standardization Provided by IHS under license with ISO Licensee=Aramco HQ/9980755100 Not for Resale, 04/16/2007 10:26:56 MDTNo reproduction or networking permitted without license from IHS -,-,-
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6、entral Secretariat at the address given below. ISO 2001 All rights reserved. Unless otherwise specified, no part of this publication may be reproduced or utilized in any form or by any means, elec- tronic or mechanical, including photocopying and microfilm, without permission in writing from either
7、ISO at the address below or ISOs mem- ber body in the country of the requester. ISO copyright office Case postale 56 CH-1211 Geneva 20 Tel. + 41 22 749 01 11 Fax + 41 22 749 09 47 E-mail copyrightiso.ch Web www.iso.ch Printed in Switzerland Copyright International Organization for Standardization Pr
8、ovided by IHS under license with ISO Licensee=Aramco HQ/9980755100 Not for Resale, 04/16/2007 10:26:56 MDTNo reproduction or networking permitted without license from IHS -,-,- ISO 16063-13:2001(E) ISO 2001 All rights reserved iii ContentsPage 1Scope .1 2Normative references .1 3Uncertainty of measu
9、rement 1 4Requirements for apparatus .2 4.1General 2 4.2Shock machine based on rigid body motion of an anvil 2 4.3Shock machine based on wave propagation inside a long thin bar .2 4.4Seismic block(s) for shock machine and laser interferometer .4 4.5Laser 4 4.6Interferometer 4 4.7Oscilloscope 7 4.8Wa
10、veform recorder with computer interface 7 4.9Computer with data-processing program 7 4.10Filters .7 4.11Other requirements 7 5Ambient conditions .8 6Preferred accelerations and pulse durations 8 7Method 8 7.1Test procedure .8 7.2Data acquisition .9 7.3Data processing .9 8Reporting the calibration re
11、sults .13 Annexes AExpression of uncertainty of measurement in calibration .14 BExplanation of the procedures16 CAlternative method of calculation of magnitude and phase shift of the complex sensitivity20 Bibliography.22 Copyright International Organization for Standardization Provided by IHS under
12、license with ISO Licensee=Aramco HQ/9980755100 Not for Resale, 04/16/2007 10:26:56 MDTNo reproduction or networking permitted without license from IHS -,-,- ISO 16063-13:2001(E) iv ISO 2001 All rights reserved Foreword ISO (the International Organization for Standardization) is a worldwide federatio
13、n of national standards bodies (ISO member bodies). The work of preparing International Standards is normally carried out through ISO technical committees. Each member body interested in a subject for which a technical committee has been established has the right to be represented on that committee.
14、 International organizations, governmental and non-governmental, in liaison with ISO, also take part in the work. ISO collaborates closely with the International Electrotechnical Commission (IEC) on all matters of electrotechnical standardization. International Standards are drafted in accordance wi
15、th the rules given in the ISO/IEC Directives, Part 3. Draft International Standards adopted by the technical committees are circulated to the member bodies for voting. Publication as an International Standard requires approval by at least 75 % of the member bodies casting a vote. Attention is drawn
16、to the possibility that some of the elements of this part of ISO 16063 may be the subject of patent rights. ISO shall not be held responsible for identifying any or all such patent rights. International Standard ISO 16063-13 was prepared by Technical Committee ISO/TC 108,Mechanical vibration and sho
17、ck, Subcommittee SC 3,Use and calibration of vibration and shock measuring instruments. ISO 16063 consists of the following parts, under the general titleMethods for the calibration of vibration and shock transducers: Part 1: Basic concepts Part 11: Primary vibration calibration by laser interferome
18、try Part 12: Primary vibration calibration by the reciprocity method Part 13: Primary shock calibration using laser interferometry Part 21: Secondary vibration calibration by comparison Annex A forms a normative part of this part of ISO 16063. Annexes B and C are for information only. Copyright Inte
19、rnational Organization for Standardization Provided by IHS under license with ISO Licensee=Aramco HQ/9980755100 Not for Resale, 04/16/2007 10:26:56 MDTNo reproduction or networking permitted without license from IHS -,-,- ISO 16063-13:2001(E) ISO 2001 All rights reserved v Introduction The shock sen
20、sitivityis determined, according to definition, as the relationship between the peak values of the accelerometer output quantity and the acceleration.is not a unique quantity but may vary depending on the duration and shape of the shock pulse and the bandwidth over which the sensitivity of the trans
21、ducer under test and the frequency response of the optional conditioning amplifier are sufficiently uniform. A unique quantity applicable for linearity tests of accelerometers is the complex sensitivity at a frequency, calculated in the frequency domain. This part of ISO 16063 makes use of data-proc
22、essing procedures which allow the magnitudeand phase shiftof the complex sensitivity to be calculated, in addition or alternatively to the shock sensitivity(cf. informative annex C). The method specified in this part of ISO 16063 is based on the absolute measurement of the time history of the motion
23、. This method fundamentally deviates from another shock calibration method which is based on the principle of the change in velocity, described in ISO 16063-1. The shock sensitivity therefore differs fundamentally from the shock calibration factor obtained by the latter method, but is in compliance
24、with the calibration factor stated in ISO 5347-41). 1)To be revised as ISO 16063-22. Ssh Ssh fn Snn Ssh Copyright International Organization for Standardization Provided by IHS under license with ISO Licensee=Aramco HQ/9980755100 Not for Resale, 04/16/2007 10:26:56 MDTNo reproduction or networking p
25、ermitted without license from IHS -,-,- Copyright International Organization for Standardization Provided by IHS under license with ISO Licensee=Aramco HQ/9980755100 Not for Resale, 04/16/2007 10:26:56 MDTNo reproduction or networking permitted without license from IHS -,-,- INTERNATIONAL STANDARDIS
26、O 16063-13:2001(E) ISO 2001 All rights reserved 1 Methods for the calibration of vibration and shock transducers Part 13: Primary shock calibration using laser interferometry 1Scope This part of ISO 16063 specifies the instrumentation and procedure to be used for primary shock calibration of rectili
27、near accelerometers, using laser interferometry to sense the time-dependent displacement during the shock. The method is applicable in a shock pulse duration rangetoand a range of peak values of to(pulse-duration dependent). The method allows the shock sensitivity to be obtained. 2Normative referenc
28、es The following normative documents contain provisions which, through reference in this text, constitute provisions of this part of ISO 16063. For dated references, subsequent amendments to, or revisions of, any of these publications do not apply. However, parties to agreements based on this part o
29、f ISO 16063 are encouraged to investigate the possibility of applying the most recent editions of the normative documents indicated below. For undated references, the latest edition of the normative document referred to applies. Members of ISO and IEC maintain registers of currently valid Internatio
30、nal Standards. ISO 5347-22,Methods for the calibration of vibration and shock pick-ups Part 22: Accelerometer resonance testing General methods ISO 16063-1,Methods for the calibration of vibration and shock transducers Part 1: Basic concepts ISO 16063-11,Methods for the calibration of vibration and
31、shock transducers Part 11: Primary vibration calibration by laser interferometry 3Uncertainty of measurement The limits of the uncertainty of shock sensitivity measurement shall be as follows: of the reading at a reference peak value ofand reference shock pulse duration ofand reference amplifier gai
32、n settings; for all values of peak acceleration and shock pulse duration. The uncertainty specifications above are valid for the calibration of acceptable precision-grade transducers (e.g. reference standard accelerometers) provided that great care is taken to keep all uncertainty components small e
33、nough to comply with the specifications (for uncertainty budgets, see annex A). In particular, the spectral energy produced by the excitation of any mode of resonance inherent in the transducer or shock machine structure during calibration must be small relative to the spectral energy contained in t
34、he frequency range of calibration. The transducer resonance testing shall be performed in accordance with ISO 5347-22. In general, this requirement might preclude the use of pulses with relatively short durations that are given in clauses 1 and 6. All users of this part of ISO 16063 shall make uncer
35、tainty budgets according to annex A to document their level of uncertainty. NOTEThe uncertainty of measurement is expressed as the expanded measurement uncertainty in accordance with ISO 16063-1 (briefly referred to as “uncertainty”). 0,05 ms10 ms102m/s2 105m/s2 1 %1 000 m/s22 ms 62 % Copyright Inte
36、rnational Organization for Standardization Provided by IHS under license with ISO Licensee=Aramco HQ/9980755100 Not for Resale, 04/16/2007 10:26:56 MDTNo reproduction or networking permitted without license from IHS -,-,- ISO 16063-13:2001(E) 2 ISO 2001 All rights reserved 4Requirements for apparatu
37、s 4.1General This clause gives specifications for the apparatus necessary to fulfil the scope of clause 1 and to obtain the uncertainties of clause 3. 4.2Shock machine based on rigid body motion of an anvil The shock machine shall be operated with a hammer (projectile) which shall be permitted to mo
38、ve and strike an anvil (target) to which the accelerometer is attached. The hammer shall impart a motion to the anvil which shall be permitted to accelerate freely and rectilinearly while the hammer shall be automatically caught. Steel springs or cushioning pads made of rubber, paper or another puls
39、e-forming material shall be placed between the hammer and the anvil to obtain the desired pulse duration and shape. The shock pulses obtained shall have a shape approximating a half-sine, half-sine squared or Gaussian acceleration shape. The resonance frequencies of the hammer and the anvil shall be
40、 at least, whereis the pulse duration. In order to avoid influences from resonances in the shock machine structure, the hammer and the anvil shall operate largely isolated from the structure. The hammer and the anvil shall be aligned with a maximum distance of between the two centrelines. The anvil
41、shall be supported in such a way that no unsymmetric forces cause rotation and deviations from rectilinear motion. The surface on which the accelerometer is to be mounted shall have a roughness value, expressed as the arithmetical mean deviation, of. The flatness shall be such that the surface is co
42、ntained between two parallel planes at a distance apart of, over the area corresponding to the maximum mounting surface of any transducer to be calibrated. The drilled and tapped hole for connecting the accelerometer shall have a perpendicular tolerance to the surface of ; i.e. the centreline of the
43、 hole shall be contained in a cylindrical zone ofdiameter and a height equal to the hole depth. NOTE 1The above requirements can be fulfilled when the anvil or both the anvil and the hammer is (are) equipped with air bearings (cf. Figure 1 and reference 1). The shock machine shown in Figure 1 allows
44、 impulses of a half-sine squared acceleration shape to be generated 6. NOTE 2Some conventional shock machines used in comparison shock calibrations in accordance with ISO 5347-4 (cf. 2 and 3) may not cause a motion which can be accurately measured by laser interferometry. 4.3Shock machine based on w
45、ave propagation inside a long thin bar The shock machine shall consist mainly of a movable element e.g. a steel ball (projectile) which shall be accelerated to strike a mitigating element (e.g. a steel ball of the same diameter) attached to a bar on which the accelerometer shall be mounted at the op
46、posite end surface. The bar shall be flexibly supported in such a way that influences from resonances in the shock machine structure are avoided. The hammer and the anvil bar shall be aligned sufficiently to meet the uncertainty requirements of clause 3. Any deviations from the rectilinear motion of
47、 the accelerometers mounting surface shall be so small, at least during the measurement period which is significant for the data acquisition (maximum:), that the stated uncertainty in calibration can be achieved. The shock machine shall be provided with a facility for triggering the data acquisition
48、 process. The surface on which the accelerometer is to be mounted shall have a roughness value, expressed as the arithmetical mean deviation, of. The flatness shall be such that the surface is contained between two parallel planes at a distance apart of, over the area corresponding to the maximum mounting surface of any transducer to be calibrated. 10/TT 0,2 mm Ra8 bits 10 bits 2 500 m/s22 ms 50 MHz1 Mbyte 1 % Copyright International Organization for Standardization Provided by IHS under license with ISO Licensee