BS 7085-1989 Guide to safety aspects of experiments in which people are exposed to mechanical vibration and shock《在人员受机械振动和冲击情况下进行实验的安全指南》.pdf
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1、BRITISH STANDARD BS 7085:1989 Guide to Safety aspects of experiments in which people are exposed to mechanical vibration and shock UDC 614.872.5BS7085:1989 This British Standard, having been prepared under the directionof the General Mechanical Engineering Standards Policy Committee, waspublished un
2、der the authorityof the Board of BSIandcomes into effect on 31August1989 BSI 11-1999 The following BSI references relate to the work on this standard: Committee reference GME/21 Draft for comment 87/74731 DC ISBN 0 580 17175 2 Committees responsible for this British Standard The preparation of this
3、British Standard was entrusted by the General Mechanical Engineering Standards Policy Committee (GME/-) to Technical Committee GME/21, upon which the following bodies were represented: British Maritime Technology British Steel Corporation Electricity Supply Industry in England and Wales Institute of
4、 Sound NOTESee Appendix A of BS6841:1987. b) the extraneous risk that malfunction or inadvertent operation of the equipment used to generate the mechanical vibration or shock may cause the subject to be exposed unintentionally to motions so severe as to cause injury or ill-health; c) the risk of inj
5、ury to the subject, the experimenter, or others in the vicinity arising from any of the following: 1) the relative motion between the vibration equipment and its surroundings; 2) mechanical or other failures; 3) falling. 3.2 Inherent risks in mechanical vibration and shock experiments The inherent r
6、isk that exposure of a subject to mechanical vibration or shock may lead to injury or ill health depends on the following two possible causes: a) using mechanical vibration or shock that is too severe in terms of magnitude or duration; NOTEInformation about magnitudes of mechanical vibration or shoc
7、k is given in3.3. b) failure to exclude from the test a subject who is medically unfit or otherwise particularly sensitive to mechanical vibration or shock. NOTEPrecautions to be taken with subjects are given in clause8. 1) Hereinafter referred to as “the subject”.BS7085:1989 2 BSI 11-1999 3.3 Sever
8、ity of mechanical vibration or shock stimulus The effects on subjects of mechanical vibration and shock depend on the magnitude, frequency content, direction of action and duration of the stimuli, all of which should be included in assessing the severity. In all cases the mechanical vibration is to
9、be measured at the interface of the subject with the vibrating surface in accordance with BS6841. Vibrations may be characterized as periodic or random and for the purpose of this standard are restricted to frequencies between0.5Hz and80Hz. Shocks may be applied with or without the presence of vibra
10、tion, with various characteristics and may be applied singly or repetitively. Figure 1 Basicentric axes of the human bodyBS7085:1989 BSI 11-1999 3 Mechanical vibration and shock should be characterized from measurements of acceleration in three mutually perpendicular axes, with the addition of a fou
11、rth measurement, for seated subjects, of the fore-and-aft (x-axis) acceleration at the interface with the backrest in accordance withA.5 of BS6841:1987 (seeFigure 1). Frequency weighting functions which reflect the different sensitivities of subjects to vibration stimuli with different axes are give
12、n inAppendix A. The use of these weighting functions enables exposure to continuous sinusoidal or random mechanical vibration, which is statistically stationary, to be assessed simply in terms of the r.m.s.value of frequency-weighted acceleration and its duration. Exposure to mechanical vibration, w
13、hose characteristics vary with time, and to mechanical shock, may be assessed in terms of a vibration dose value VDV (in ms 1.75 ) which is calculated from the following equation: where For mechanical vibrations which are statistically stationary the estimated vibration dose value eVDV (in ms 1.75 )
14、 may be approximated from the following equation (seeA.4 of BS6841:1987): where For mechanical vibration which comprises significant components in more than one direction, a total vibration dose value can be calculated as the fourth root of the sum of the fourth powers of vibration dose values in ea
15、ch axis. Alternatively, where r.m.s.values have been calculated, a convenient approximation to the total vibration magnitude may be determined as the square root of the sums of the squares of the individual ponents (seeTable 1). 3.4 Extraneous risks in mechanical vibration and shock experiments 3.4.
16、1 Equipment malfunction. Many vibrating devices used in experiments have a large quantity of available or stored energy. An inherent problem in the design of vibration systems is that the subject may be exposed to unexpected or frightening transients, or at worst, to potentially dangerous magnitudes
17、 of mechanical vibration or shock as a result of a malfunction. In shock experiments, the subject is either brought suddenly to rest after slow acceleration to a specified velocity, or accelerated suddenly from rest. There is an attendant risk that equipment malfunction could lead to dangerous magni
18、tudes of shock. Equipment design should be such that, in the event of malfunction or emergency stop procedures, the subject should not be exposed to changes in the force environment of hazardous intensity or duration. Equipment should be designed so that no failure could result in magnitudes of mech
19、anical vibration or shock producing vibration dose values in excess of15ms 1.75 , unless the experiment is designed to study the effects of higher magnitudes. For such experiments, the magnitude during failure conditions should be only slightly in excess of those being studied. 3.4.2 Physical contac
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